Yuichi
Negishi
*ab,
Nobuyuki
Shimizu
a,
Kanako
Funai
a,
Ryo
Kaneko
a,
Kosuke
Wakamatsu
a,
Atsuya
Harasawa
a,
Sakiat
Hossain
a,
Manfred E.
Schuster
c,
Dogan
Ozkaya
c,
Wataru
Kurashige
d,
Tokuhisa
Kawawaki
ab,
Seiji
Yamazoe
*e and
Shuhei
Nagaoka
*d
aDepartment of Applied Chemistry, Faculty of Science, Tokyo University of Science, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan. E-mail: negishi@rs.kagu.tus.ac.jp
bPhotocatalysis International Research Center, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan
cJohnson Matthey Technology Centre, Blounts Court, Sonning Common, Reading RG4 9NH, UK
dJohnson Matthey Japan, G.K., 5123-3, Kitsuregawa, Sakura, Tochigi 329-1492, Japan. E-mail: Shuhei.Nagaoka@mattheyasia.com
eDepartment of Chemistry, Graduate School of Science, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji-shi, Tokyo 192-0397, Japan. E-mail: yamazoe@tmu.ac.jp
First published on 3rd December 2019
Although Pt is extensively used as a catalyst to purify automotive exhaust gas, it is desirable to reduce Pt consumption through size reduction because Pt is a rare element and an expensive noble metal. In this study, we successfully loaded a Pt17 cluster on γ-alumina (γ-Al2O3) (Pt17/γ-Al2O3) using [Pt17(CO)12(PPh3)8]Cln (n = 1, 2) as a precursor. In addition, we demonstrated that Pt is not present in the form of an oxide in Pt17/γ-Al2O3 but instead has a framework structure as a metal cluster. Moreover, we revealed that Pt17/γ-Al2O3 exhibits higher catalytic activity for carbon monoxide and propylene oxidation than γ-Al2O3-supported larger Pt nanoparticles (PtNP/γ-Al2O3) prepared using the conventional impregnation method. Recently, our group discovered a simple method for synthesizing the precursor [Pt17(CO)12(PPh3)8]Cln. Furthermore, Pt17 is a Pt cluster within the size range associated with high catalytic activity. By combining our established synthesis and loading methods, other groups can conduct further research on Pt17/γ-Al2O3 to explore its catalytic activities in greater depth.
Many attempts have been made to develop catalysts without Pt. However, previous studies have implied that the activity and durability of Pt are superior to those of non-precious metals. To reduce the amount of Pt consumed while taking advantage of its characteristic features, it is essential to improve its activity and performance per unit weight of the catalyst. The size reduction of Pt nanoparticles/clusters (hereinafter: Ptn clusters) increases the proportion of surface atoms2,3 and enables the creation of new geometrical/electronic structures;4–10 thus, this approach can efficiently reduce Pt consumption.11–13
Meanwhile, the geometrical/electronic structures and chemical properties of Ptn clusters in the fine size range vary considerably depending on the number of constituent atoms.14 Therefore, it is important to load Ptn clusters with a controlled number of constituent atoms on a substrate to create a highly active supported Pt catalyst using fine Ptn clusters while elucidating the catalytic activity and performance of the clusters. Using a vacuum device with a mass selector,2,6,10,15–19 it is possible to load controlled Ptn clusters onto a substrate. In fact, magnesium-oxide-supported Ptn clusters (Ptn/MgO; n = 8–20) and titanium-dioxide-supported Ptn/TiO2 (n = 4, 7–10, 15) have been prepared with precisely controlled numbers of Pt atoms using these types of experiments. These studies also revealed that fine supported Ptn clusters exhibit high catalytic activity for the oxidation of carbon monoxide (CO).2,19 However, for the practical use of supported Pt catalysts, issues remain regarding device manufacturing costs and loading efficiency for the preparation of supported Ptn clusters using such vacuum equipment.
Recently, it has become possible to precisely synthesize various noble-metal and noble-metal-alloy clusters with atomic accuracy.20–49 Ptn clusters can be synthesized with atomic accuracy using CO as a ligand or two types of ligand, CO and phosphine.48 In addition, Ptn clusters can be precisely synthesized using special dendrimers as templates.50,51 When these Ptn clusters are adsorbed on a substrate followed by the removal of the ligands, Ptn clusters with a controlled number of constituent atoms can be loaded on the substrate without the issues of device construction cost and loading efficiency (Fig. 1). However, currently, there are few examples of controlled loading of Ptn clusters on a substrate using this approach. For the synthesis of the former ligand-protected Ptn clusters, it is essential to carry out the reaction under a CO atmosphere. For the synthesis of the latter dendrimer-protected Ptn clusters, a special dendrimer synthesis technique is needed. Therefore, few research groups are capable of conducting these precise syntheses, and fundamental and applied research on fine supported Ptn clusters is currently limited.
We recently discovered a very simple method for synthesizing Pt17 clusters protected with CO and triphenylphosphine (PPh3) ([Pt17(CO)12(PPh3)8]Cln; n = 1, 2; Fig. 2(a)).52 In our synthesis method, first, the Ptn(CO)m(PPh3)l cluster, which is mainly composed of [Pt17(CO)12(PPh3)8]Cln, is prepared by mixing the reagents and heating the solvent in the atmosphere. Then, the main product, [Pt17(CO)12(PPh3)8]Cln, is separated from the obtained mixture with high purity using the difference in solubility. This method does not require special synthesis equipment or dendrimer synthesis techniques. If we could establish the loading method of the Pt17 cluster using [Pt17(CO)12(PPh3)8]Cln as a precursor, many research groups would be able to obtain fine supported Pt17 catalysts.
Fig. 2 (a) Geometrical structure of [Pt17(CO)12(PPh3)8]+ determined by single-crystal X-ray crystallography. The geometrical structure (a) was reproduced from ref. 51. (b) Positive-ion ESI mass spectrum of [Pt17(CO)12(PPh3)8]Cln synthesized in this work. The spectrum indicates that both [Pt17(CO)12(PPh3)8]Cln (n = 1, 2) are contained in this sample, similar to the previous work.52 (c) TEM and (d) HAADF-STEM images of [Pt17(CO)12(PPh3)8]Cln. In (c), the green circles indicate the particles and the histogram estimated from the TEM images is also provided. Copyright 2017 American Chemical Society. |
In this study, the following three goals were addressed with the final objective of using supported Ptn clusters as catalysts to treat automotive exhaust gas: (i) establishment of a precise loading method of Pt17 on γ-alumina (γ-Al2O3); (ii) structural analysis of the obtained Pt17/γ-Al2O3; and (iii) evaluation of the catalytic activity of Pt17/γ-Al2O3 against the oxidation reaction of CO and propylene (C3H6). As a result, we successfully determined the conditions for loading Pt17 on γ-Al2O3 while preserving the size of Pt17 (Fig. 1). We observed that the supported Pt17 is not present in the form of an oxide53 but has a framework structure as a metal cluster in the obtained Pt17/γ-Al2O3. Furthermore, Pt17/γ-Al2O3 exhibited higher catalytic activity against the oxidation of CO and C3H6 than γ-Al2O3-supported larger Pt nanoparticles (PtNP/γ-Al2O3) prepared using the conventional impregnation method.
The resulting [Pt17(CO)12(PPh3)8]Cln was first adsorbed onto γ-Al2O3 (Fig. 1(b)). In an aprotic solvent, the metal oxide has a permanent dipole moment on the surface.55 As reported by Tsukuda et al., when this surface comes into contact with a metal cluster containing a functional group with a high dielectric constant (e.g., a phenyl group) in the ligand, an induced dipole moment is generated in the ligand layer, and the metal clusters are adsorbed on the surface of the metal oxide via a dipole–induced dipole interaction.56 In the [Pt17(CO)12(PPh3)8]Cln used in this study, the ligand layer contained a large amount of phenyl groups, and [Pt17(CO)12(PPh3)8]Cln was thus adsorbed onto γ-Al2O3via a dipole–induced dipole interaction. Dichloromethane was used as the aprotic solvent. The concentration of [Pt17(CO)12(PPh3)8]Cln in solution was carefully controlled by inductively coupled plasma mass spectrometry (ICP-MS) such that the weight of Pt17 was 0.15 wt% relative to γ-Al2O3. The solution changed from brown to colorless and transparent after 2 h of stirring, indicating that practically all of the [Pt17(CO)12(PPh3)8]Cln was adsorbed onto γ-Al2O3 (Pt17(CO)12(PPh3)8/γ-Al2O3).
The particle diameter of Pt17(CO)12(PPh3)8/γ-Al2O3 obtained using this approach was estimated by HAADF-STEM measurement. In the HAADF-STEM image in Fig. 3(a), particles (0.94 ± 0.16 nm) with sizes similar to that of [Pt17(CO)12(PPh3)8]Cln (1.0 ± 0.2 nm; Fig. 2(d) and S2†) were observed with a narrow distribution (Fig. S3†). The HAADF-STEM image of Pt17(CO)12(PPh3)8/γ-Al2O3 (Fig. 3(a)) shows that it contained many particles with shapes similar to that of the Pt17 core of the precursor [Pt17(CO)12(PPh3)8]Cln (Fig. 3(b)). In the diffuse reflection (DR) spectrum of Pt17(CO)12(PPh3)8/γ-Al2O3, a peak structure similar to that of [Pt17(CO)12(PPh3)8]Cln was observed (Fig. 4(a) and (b)). These results indicate that aggregation of Pt17(CO)12(PPh3)8 hardly occurred during the adsorption process and that Pt17(CO)12(PPh3)8 after adsorption retained the geometrical/electronic structure of the precursor [Pt17(CO)12(PPh3)8]Cln.
Fig. 3 (a) HAADF-STEM image of Pt17(CO)12(PPh3)8/γ-Al2O3. (b) Pt17-core structure (two-angle views) of [Pt17(CO)12(PPh3)8]Cln (Fig. 2(a)) on the same scale as (a) and (c). (c) HAADF-STEM image of Pt17/γ-Al2O3. In (a) and (c), the histogram and average diameters estimated from the various HAADF-STEM images (Fig. S3 and S6†) are also included. |
Fig. 4 DR spectra of (a) [Pt17(CO)12(PPh3)8]Cln, (b) Pt17(CO)12(PPh3)8/γ-Al2O3, and (c) Pt17/γ-Al2O3. For (b) and (c), the spectra were obtained by the subtraction of γ-Al2O3. The DR spectral profile of [Pt17(CO)12(PPh3)8]Cln (a) differs slightly from that reported in our previous work.52 This difference likely results from the different ratios of the two kinds of charged clusters, [Pt17(CO)12(PPh3)8]Cln (n = 1 or 2), in the two studies. |
Then, the PPh3 ligands were removed from Pt17(CO)12(PPh3)8/γ-Al2O3 by calcination57–61 (Fig. 1(c)). Based on thermogravimetric mass spectrometry (TG-MS) analysis, a temperature of approximately 400 °C is required for PPh3 removal (Fig. S4†).62 Thus, PPh3 was removed from the Pt17 cluster by calcination at 500 °C. In the DR spectra of the sample after calcination (Fig. 4(c)), the peaks of [Pt17(CO)12(PPh3)8]Cln (Fig. 4(a)) and Pt17(CO)12(PPh3)8/γ-Al2O3 (Fig. 4(b)) were not observed. In the X-ray photoelectron spectrum after calcination (Fig. S5†), the P 2p peak was not observed. In the HAADF-STEM image of the sample after calcination (Fig. 3(c)), particles (1.07 ± 0.24 nm) with sizes similar to that of Pt17(CO)12(PPh3)8/γ-Al2O3 (0.94 ± 0.16 nm; Fig. 3(a)) were observed with a narrow distribution (Fig. S6†). These results indicate that the PPh3 ligands were removed from the cluster by calcination and that Pt17 did not aggregate during this process. Pt forms a relatively strong bond with O compared with other noble metals (318.4 ± 6.7 kJ mol−1 for Pt–O vs. 223 ± 21.1 kJ mol−1 for Au–O).63 Furthermore, as γ-Al2O3 has a complicated structure in which Al atoms are arranged octahedrally or tetrahedrally, cationic sites are present because of the surface defects in γ-Al2O3.64 Pt clusters could be strongly immobilized on γ-Al2O3 by the interaction between Pt atoms and these cationic sites.53 For these reasons, it is considered that Pt17 did not aggregate on γ-Al2O3 during calcination. To confirm the weight of Pt loaded on γ-Al2O3, Pt17/γ-Al2O3 was mixed with aqua regia, and the amount of dissolved Pt was measured using ICP optical emission spectroscopy (ICP-OES). The results confirmed that 0.15 wt% Pt was actually loaded on γ-Al2O3. The results of temperature-programmed reaction measurements indicate that the surface of the supported Pt17 was covered by CO at normal temperature (Fig. 1(d), S7 and S8†). This result is most likely due to the existence of uneliminated CO (Fig. 1(c)) as well as the adsorption of CO from the atmosphere.
The Pt L3-edge X-ray absorption near-edge structure (XANES) spectra of [Pt17(CO)12(PPh3)8]Cln, Pt17(CO)12(PPh3)8/γ-Al2O3, and Pt17/γ-Al2O3 are shown in Fig. 5(a) together with those of Pt foil and PtO2 for comparison. The white-line intensities of [Pt17(CO)12(PPh3)8]Cln, Pt17(CO)12(PPh3)8/γ-Al2O3, and Pt17/γ-Al2O3 are similar to that of Pt foil and very different from that of PtO2. This result indicates that Pt is not present as an oxide in Pt17.53 Among the three samples, the white-line intensity increases in the order of [Pt17(CO)12(PPh3)8]Cln → Pt17(CO)12(PPh3)8/γ-Al2O3 → Pt17/γ-Al2O3. This result indicates that the number of holes in the d orbital of Pt17 increases, namely the electron density of Pt17 decreases, in this order.
Fig. 5 (a) Pt L3-edge XANES and (b) Pt L3-edge FT-EXAFS spectra of [Pt17(CO)12(PPh3)8]Cln, Pt17(CO)12(PPh3)8/γ-Al2O3, and Pt17/γ-Al2O3 together with those of Pt foil and PtO2 for comparison. (c) and (d) two proposed structures for Pt17 on γ-Al2O3, which were estimated based on the HAADF-STEM images (Fig. 3(c) and S6†) of Pt17/γ-Al2O3 (Fig. S11†). In (b), the peak at ∼2.3 Å in the spectrum of Pt foil is attributed to the satellite peak of the Pt–Pt bond. In (c) and (d), both top and side views are shown. |
Fig. 5(b) shows the Pt L3-edge Fourier-transform extended X-ray absorption fine structure (FT-EXAFS) spectra of [Pt17(CO)12(PPh3)8]Cln, Pt17(CO)12(PPh3)8/γ-Al2O3, and Pt17/γ-Al2O3 (Tables S1–S3 and Fig. S9†). In the FT-EXAFS spectrum of [Pt17(CO)12(PPh3)8]Cln, the peaks attributed to the Pt–C and Pt–P bonds appear at ∼1.7 and ∼2.3 Å, respectively. For Pt17(CO)12(PPh3)8/γ-Al2O3, the intensity of the peak at ∼1.7 Å increased and that at ∼2.3 Å decreased, and the peak attributed to the Pt–Pt bond appeared at ∼2.8 Å. As described above, there is no significant difference in the optical absorption between [Pt17(CO)12(PPh3)8]Cln and Pt17(CO)12(PPh3)8/γ-Al2O3 (Fig. 4(a) and (b)). Therefore, it is assumed that the Pt17 cluster maintains the metal-core structure as a whole even during adsorption (Fig. 3(a) and (b)). However, the FT-EXAFS spectrum indicates that the adsorption causes a slight change in the structure of the ligand layer that covers Pt17. For the appearance of the Pt–Pt bond in the spectrum, a plausible explanation is that the variation in the Pt–Pt bond length (Fig. S10†) decreases or the fluctuation of the Pt–Pt bond decreases65 with adsorption on the substrate. The decrease in the electron density of the d orbital of Pt17 (Fig. 5(a)) caused by adsorption can also likely be attributed to the structural change of the ligand layer. In the spectrum of Pt17/γ-Al2O3 after calcination, a peak at ∼2.8 Å clearly appears, and its satellite peak (in the FT-EXAFS spectrum of the Pt foil in Fig. 5(b)) is also observed at ∼2.3 Å.66 This result indicates that the variation in the Pt–Pt bond length and/or the fluctuation of the Pt–Pt bond further decrease with the PPh3 removal and/or the structural change of the Pt17 cluster from the icosahedral-based structure (Fig. 2(a)) to the structure shown in Fig. 5(c) and (d) (see below). In this spectrum, a peak was also observed at ∼1.7 Å. As described above, the surface of supported Pt17 is covered by CO at normal temperature. The peak at ∼1.7 Å is attributed to the generated Pt–C or Pt–O bond at the Pt17/γ-Al2O3 interface.
Thus, it was observed that Pt does not form an oxide53 and that Pt17 has a framework structure like a metal cluster in Pt17/γ-Al2O3. Based on the HAADF-STEM image, the supported Pt17 is assumed to have a bi-layer2 or tri-layer structure, as shown in Fig. 5(c), (d) and S11.† Previous studies have suggested that CO and O2 are activated on the terrace Pt and step Pt, respectively, during the oxidation reaction of CO.2,3,18Fig. 5(c) and (d) show that most of the terrace Pt is located near the step Pt in Pt17/γ-Al2O3. Thus, the reaction of CO and O2, i.e., the oxidation of CO, is expected to proceed effectively over Pt17/γ-Al2O3.
Fig. 6 (a) Representative HAADF-STEM image and (b) histogram estimated from various HAADF-STEM images of PtNP/γ-Al2O3 prepared for comparison. |
The obtained Pt17/γ-Al2O3 and PtNP/γ-Al2O3 were examined for their catalytic activity against the oxidation of CO and C3H6, which are the main components in automobile gas.1 In an actual automobile, the catalysts are coated on a honeycomb substrate made of cordierite ceramic. Thus, in this study, Pt17/γ-Al2O3 and PtNP/γ-Al2O3 were coated on a honeycomb substrate to evaluate their catalytic performance in a state similar to the actual vehicle mounting conditions (Scheme S2†).
Scheme 1 Schematic illustration of the estimation of CO and C3H6 conversions over Pt17/γ-Al2O3 or PtNP/γ-Al2O3 coated on a cordierite honeycomb substrate. |
Fig. 7(a) shows the CO conversion for each catalyst (Pt17/γ-Al2O3 or PtNP/γ-Al2O3) estimated using this approach. When PtNP/γ-Al2O3 was used as the catalyst, the catalytic activity started to appear at approximately 270 °C, and the conversion reached 50% at approximately 350 °C (light-off temperature) and nearly 100% at approximately 370 °C. However, when Pt17/γ-Al2O3 was used, the catalytic activity started to manifest at approximately 240 °C, and the conversion reached 50% at approximately 330 °C and almost 100% at approximately 350 °C. These results indicate that Pt17/γ-Al2O3 exhibits higher catalytic activity at each temperature than PtNP/γ-Al2O3 and thus that Pt17/γ-Al2O3 can treat CO at lower temperatures than PtNP/γ-Al2O3. Currently, the issue of enhanced activity of exhaust-gas-treating catalysts at low temperatures must be overcome with the spread of vehicles that frequently stop and restart their engines (e.g., hybrid vehicles).1 These results strongly suggest that Pt17/γ-Al2O3 could be used as an exhaust gas-treating catalyst to overcome this issue.
The higher activity of Pt17/γ-Al2O3 than PtNP/γ-Al2O3 is considered to be associated with their respective geometrical structures.67 Although the geometrical structures of Pt17/γ-Al2O3 and PtNP/γ-Al2O3 before the reaction experiments are shown in Fig. 5 and 6, these geometrical structures should change as the catalytic reaction progresses and have not yet been elucidated.68 However, there should be more combinations composed of the terrace and step Pt in Pt17/γ-Al2O3 than in PtNP/γ-Al2O3 (Fig. 5(c) and (d)). These geometrical effects appear to make the reaction between CO and O2 more likely to occur in Pt17/γ-Al2O3, resulting in higher CO conversion of Pt17/γ-Al2O3 at any temperature. In addition, Pt17 in Pt17/γ-Al2O3 should be more susceptible to the fluctuation of the geometrical/electronic structure than PtNP in PtNP/γ-Al2O3. The ease of fluctuation of their geometrical/electronic structures may also contribute to the high activity of Pt17/γ-Al2O3.9 Furthermore, CO adsorbed on fine Ptn supported clusters generally has a longer C–O bond than that adsorbed on the larger Ptn supported nanoparticles, which promotes the oxidation reaction.69 In addition to the geometric factors, it is assumed that such a difference in CO activation caused by the difference in electronic states between the two supported clusters also contributes to the high activity of Pt17/γ-Al2O3.
Fig. 7(b) shows the C3H6 conversion for each catalyst (Pt17/γ-Al2O3 or PtNP/γ-Al2O3) estimated using this approach. When PtNP/γ-Al2O3 was used as a catalyst, the catalytic activity started to manifest at approximately 160 °C, and the conversion reached 50% at approximately 245 °C and nearly 100% at approximately 260 °C. However, when Pt17/γ-Al2O3 was used, the catalytic activity started to manifest at approximately 130 °C, and the conversion reached 50% at approximately 225 °C and nearly 100% at approximately 250 °C. These results indicate that Pt17/γ-Al2O3 exhibits higher catalytic activity at each temperature than PtNP/γ-Al2O3 for oxidizing C3H6. Currently, the mechanism of C3H6 oxidation is not as well understood as that of CO oxidation.70 Therefore, it is difficult to discuss the origin of the difference between the two activities. However, there should be a large difference between Pt17/γ-Al2O3 and PtNP/γ-Al2O3 in the number of surface Pt atoms that can participate in the reaction. It appears that this factor is responsible for the difference in activity of the two types of catalysts.
Fig. 8(a) shows the CO conversion of each catalyst (Pt17/γ-Al2O3 or PtNP/γ-Al2O3) after the aging treatment. The CO conversion rate decreased significantly for both catalysts compared with that before the aging treatment (Fig. 7(a)). A similar phenomenon was observed for the C3H6 conversion. These results indicate that the previously described procedure results in deterioration of the performance of both catalysts. However, comparing the conversion over Pt17/γ-Al2O3 and PtNP/γ-Al2O3, the use of Pt17/γ-Al2O3 resulted in higher conversion than the use of PtNP/γ-Al2O3 for both reactions. This result indicates that Pt17/γ-Al2O3 exhibits higher activity than PtNP/γ-Al2O3 even after the aging treatment.
The decrease in activity after aging is generally induced by the aggregation of the supported Pt catalyst.12,71 In fact, the aggregation of the Pt catalyst was observed after the aging treatment for both Pt17/γ-Al2O3 and PtNP/γ-Al2O3 (Fig. S12†). However, the average particle size of Pt17/γ-Al2O3 and PtNP/γ-Al2O3 after the aging treatment was 25.3 ± 19.4 and 77.5 ± 29.9 nm, respectively. Thus, the average particle size of the former was smaller than that of the latter even after the aging treatment. It is considered that because the original Pt17/γ-Al2O3 had a smaller particle size than the original PtNP/γ-Al2O3, Pt17/γ-Al2O3 had a smaller average particle size than PtNP/γ-Al2O3 after aggregation, resulting in its higher activity even after the aging treatment.
MALDI mass spectra were collected using a spiral time-of-flight mass spectrometer (JEOL, JMS-S3000) with a semiconductor laser. DCTB76 was used as the MALDI matrix (cluster:matrix = 1:1000).
TEM images were recorded with a JEM-2100 electron microscope (JEOL) operating at 200 kV, typically using a magnification of 600000.
HAADF-STEM images were recorded using a JEOL ARM200CFE fitted with an aberration corrector. The catalyst powders of Pt17/γ-Al2O3 or PtNP/γ-Al2O3 were ground between two glass slides and dusted onto a holey carbon-coated Cu TEM grid.
DR spectra were acquired at ambient temperature using a V-670 spectrometer (JASCO). The wavelength-dependent optical data (I(w)) were converted to the energy-dependent data (I(E)) using the following equation that conserved the integrated spectral areas: I(E) = I(w)/|∂E/∂w| ∝ I(w) × w2.
ICP-MS was performed using an Agilent 7500c spectrometer (Agilent Technologies, Tokyo, Japan). Bi was used as the internal standard. The ICP-MS measurements were performed for the supernatant obtained after mixing [Pt17(CO)12(PPh3)8]Cln with γ-Al2O3 to estimate the unadsorbed Pt content. The adsorption efficiency and the Pt amount on γ-Al2O3 were estimated using this value.
ICP-OES was performed using an Agilent Technologies 700 series spectrometer to determine the Pt content in Pt17/γ-Al2O3 or PtNP/γ-Al2O3 after completely dissolving the sample using aqua regia.
TG-MS was performed with an STA 2500 Regulus (NETZSCH) and a JMS-Q 1500GC (JEOL) at a heating rate of 5 °C min−1 under an Ar atmosphere over the temperature range 25–900 °C using ∼3 mg sample of Pt17(CO)12(PPh3)8/γ-Al2O3.
XPS data were collected using an electron spectrometer (JEOL, JPS-9010MC) equipped with a chamber at a base pressure of ∼2 × 10−8 Torr. X-rays from the Mg-Kα line (1253.6 eV) were used for excitation.
Pt L3-edge XAFS measurements were performed at beamline BL01B1 of the SPring-8 facility of the Japan Synchrotron Radiation Research Institute (proposal numbers 2018B1422 and 2019A0944). The incident X-ray beam was monochromatized using a Si(111) double-crystal monochromator. As references, the XAFS spectra of Pt foil and solid PtO2 were recorded in transmission mode using ionization chambers. The Pt L3-edge XAFS spectra of the samples were measured in fluorescence mode using a 19-element Ge solid-state detector at room temperature. The X-ray energies for the Pt L3-edges were calibrated using Au foil. The XANES and EXAFS spectra were analyzed using the xTunes program77 as follows. The χ spectra were extracted by subtracting the atomic absorption background using cubic spline interpolation and normalized to the edge height. The normalized data were used as the XANES spectra. The k3-weighted χ spectra in the k range 3.0–14.0 Å−1 for the Pt L3-edge were Fourier transformed into r space for structural analysis. The curve fitting analysis was performed in the range of 1.2–3.0 Å for the Pt L3-edge. In the curve fitting analysis, the phase shifts and backscattering amplitude function of Pt–C, Pt–P, and Pt–Pt were calculated using the FEFF8.5L program.
Footnote |
† Electronic supplementary information (ESI) available: Data of XAFS analysis, protocols, MALDI mass spectra, HAADF-STEM images, the XPS spectrum, the TPR curve, EXAFS curves of [Pt17(CO)12(PPh3)8]Cln, Pt17(CO)12(PPh3)8/γ-Al2O3, or Pt17/γ-Al2O3. See DOI: 10.1039/c9na00579j |
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