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Improving the electrocatalytic properties of Pd-based catalyst for direct alcohol fuel cells: effect of solid solution


The tolerance of the electrode against the CO species absorbed upon the surface presents the biggest dilemma of the alcohol fuel cells. Here we report for the first time that the inclusion of (Zr, Ce)O2 solid solution as the supporting material can significantly improve the anti-CO-poisoning as well as the activity of Pd/C catalyst for ethylene glycol electro-oxidation in KOH medium. In particular, the physical origin of the improved electrocatalytic properties has been unraveled by first principle calculations. The 3D stereoscopic Pd cluster on the surface of (Zr, Ce)O2 solid solution leads to weaker Pd-C bonding and smaller CO desorption driving force. These results support that the Pd/ZrO2-CeO2/C composite catalyst could be used as a promising effective candidate for direct alcohol fuel cells application.


Direct alcohol fuel cells (DAFCs) have been attracted great attention on their potential application in the portable electronics and automobile industries1. Among various liquid fuels, the methanol is volatile and relatively toxic, and ethanol has been recognized as the most suitable fuel as it is a sustainable and carbon-neutral transportation fuel2. However, it is difficult to break the C-C bond in ethanol at temperature lower than 100 °C, and the main product of ethanol oxidation reaction is acetate. As such, the electron transfer rate of ethanol in the alkaline DAFCs is only 33%3, 4. Ethylene glycol (EG) is a good choice to replace ethanol because the main product of the EG oxidation is oxalate5, 6, such that the ETR reaches 80%, which is much higher than that of ethanol in the alkaline DAFCs4. Also, EG has superior energy density (7.56 kWh L−1), higher boiling point (198 °C) and could be produced from biomass in great quantities7,8,9, which makes it as an appealing candidate for fuel cells application.

Pt-based catalysts have been investigated extensively as good electrocatalysts for low temperature fuel cells, especially for its acidic-resistant property10. However, compared to Pt electrocatalyst, Pd is more abundant, less expensive, and could promote EG oxidation more efficiently in alkaline media11, 12. A lot of efforts have been done to prepare the Pd-base catalysts with high catalytic activity and anti-CO-poisoning for alcohol electro-oxidation. In addition to the alloying approach11, 13,14,15,16, oxide-modified Pd has been reported to be superior to Pd/C catalyst for alcohol oxidation17,18,19,20,21,22. For instance, Li et al. reported that the addition MgO into Pd/C catalysts could significantly improve the reaction activity and the poisoning resistance for ethanol electro-oxidation due to the synergistic effect between Pd and MgO19.

CeO2 is as a well-known promoter in noble metal-based combustion catalysts. In addition, ZrO2 is always used as the support of Pt for water-gas shift in low temperature23,24,25. In recent studies, CeO2 26, 27 and ZrO2 28,29,30 have attracted increasing interests as the support of Pt or Pd and showed excellent catalytic activity. The CexZr1−xO2 system has also been investigated because that the thermal stability, redox property and oxygen storage capacity could be improved by the addition of ZrO2 to CeO2 31,32,33,34,35. However, there is few work reported about ZrO2-CeO2 mixed oxides as support materials on the EG electrocatalytic performance of Pd/C catalysts in the literatures. This prompts us to carry out an extensive and systematic investigation on this topic, which is of great interest and importance.

In this study, Pd/C, Pd/ZrO2/C, Pd/CeO2/C and Pd/ZrO2-CeO2/C composite catalysts have been prepared and characterized. The effect of the solid solution of ZrO2-CeO2 binary oxides as support materials on the electrocatalytic performance of Pd-based catalysts has been inverstigated. The physical origin of the good anti-CO-poisoning property of Pd4/ZrO2-CeO2 (111) composite catalyst has been unraveled based on first principle calculations as well.


Structural characterization

The TEM images of different catalysts are shown in Fig. 1a–d. It is clearly that Pd nanoparticles of all catalysts are uniform and monodisperse. The average size of Pd is 4.8 nm for Pd/C, 4.1 nm for Pd/CeO2/C, 4.6 nm for Pd/ZrO2/C, and 4.0 nm for Pd/ZrO2-CeO2/C, respectively, as shown in Fig. 1a–d, consistent with that calculated on XRD data (in Fig. S1). It is noticed that the particle size of Pd changes more significantly with the addition of CeO2 than ZrO2 in this work. Similar results have been reported in Pt catalysts modified by Ce0.6Zr0.4O2 31, 32.

Figure 1

TEM images of different catalysts, for (a) Pd/C, (b) Pd/ZrO2/C, (c) Pd/CeO2/C and (d) Pd/ZrO2-CeO2/C. Insets show the corresponding size distribution in (a,b,c) and (d), respectively. (e,f,g) and (h) are the HRTEM images for (a,b,c) and (d), respectively.

It is observed that some grains with a d-spacing of 0.227 nm from the HRTEM images of all catalysts in Fig. 1e–h, which is assigned for the (111) plane of cubic Pd. And the d-spacing of some grains is 0.276 nm in Pd/CeO2/C (Fig. 1g), corresponding for the (200) plane of CeO2. While the d-spacing of some grains in Pd/ZrO2-CeO2/C (Fig. 1h) turns out to be 0.274 nm, which is smaller than that of Pd/CeO2/C. This could be related to the replacement of Ce4+ ions by Zr4+ ions, which results in a shrinking of the lattice volume of the solid. Based on the HRTEM results, one can confirm that the addition of 50% ZrO2 contributes to the formation of (Zr, Ce)O2 solid solution in present work.

XPS was employed to investigate the nature of surface species for the catalysts. Figure 2 shows the XPS spectra of Zr 3d and Ce 3d in different species before and after Pd-loading. It is evident that the binding energy of Zr 3d5/2 slightly increases from 182.3 eV for ZrO2/C to 182.5 eV for Pd/ZrO2/C (Fig. 2a); while the binding energy of Ce 3d5/2 changes from 883.1 eV for CeO2/C to 883.6 eV for Pd/CeO2/C (Fig. 2b), which reveals the effect of Pd-loading on the electronic structure of Zr 3d or Ce 3d. Similar change in binding energy has been observed in Zr 3d5/2 (Zr 3d3/2) as well as Ce 3d5/2 for ZrO2-CeO2/C after Pd-loading, as shown in Fig. 2c–d. The presence of ZrO2-CeO2 in the vicinity of Pd nanoparticles could be beneficial for the EG and CO oxidation36.

Figure 2

XPS spectra of Zr 3d and Ce 3d in different species before and after Pd-loading, (a) Zr 3d for ZrO2/C and Pd/ZrO2/C, (b) Ce 3d for CeO2/C and Pd/CeO2/C, (c) Zr 3d and (d) Ce 3d for ZrO2-CeO2/C and Pd/ZrO2-CeO2/C, respectively.

Moreover, the interaction between Zr and Ce was determined by the XPS analysis. It is found the Zr 3d5/2 peak of ZrO2-CeO2/C (Fig. 2c) shifts negatively about 0.1 eV compared to that of ZrO2/C (Fig. 2a), and the Ce 3d5/2 peak of ZrO2-CeO2/C (Fig. 2d) shifts negatively about 0.1 eV compared to that of CeO2/C (Fig. 2b). It indicates that there was an electronic interaction between the ZrO2 and CeO2, which could play an important role in catalytic reaction and the activation of both dispersed metal and oxide matrix during electrode process37. The electron cloud density of Pd could be changed by ZrO2-CeO2/C supporting, and a synergetic effect could be yielded to improve the catalytic activity of Pd catalyst.

The XPS spectra of Pd 3d in different catalysts are shown in Fig. 3. It shows that the peaks corresponding for Pd 3d5/2 (~335.7 eV) and Pd 3d3/2 (~341.0 eV) core levels can be ascribed to Pd and PdOy (0 < y < 2) species, respectively38, 39. It is obviously that both Pd metal and PdOy can be observed on the surface of prepared catalysts. The ratio of Pd: PdOy is respectively calculated to be 1.2, 1.4, 2.0 and 2.3 for Pd/C, Pd/CeO2/C, Pd/ZrO2/C and Pd/ZrO2-CeO2/C. As reported in the literature33, CeO2 can act as an oxygen storage reservoir, which gives lattice oxygen to Pd and stabilizes Pd in an oxidized form. Therefore, the increased metallic Pd content can be mainly related to (Zr, Ce)O2 solid solution.

Figure 3

XPS spectra of Pd 3d for different catalysts.

In addition, the binding energy of Pd 3d5/2 shifts positively from 335.65 eV for Pd/C to 335.70 eV for Pd/CeO2/C, and to 335.74 eV for Pd/ZrO2-CeO2/C. Combining with the XPS results in Zr 3d, Ce 3d and Pd 3d (in Figs 2 and 3), it can conclude that strong interaction exists between Pd and oxides, especially for the addition of (Zr, Ce)O2 solid solution. Moreover, the atom ratio of Pd: Zr: Ce is measured about 6.49: 0.98: 1.02 for Pd/ZrO2-CeO2/C catalyst, while the values are about 6.51: 1.92: 0 and 6.45: 0: 2.01 for Pd/ZrO2/C and Pd/CeO2/C respectively, indicating that Pd has been sucessfully loaded in the oxide support and the atom ratio of Zr: Ce is nearly 1: 1 for ZrO2-CeO2 solid solution.

Electrochemical activity and stability

Figure 4 shows the cyclic voltammograms of different catalysts in 1 M KOH solution. It is known that the position and size of anodic peak often change with the modification of Pd catalyst. In general, the anodic peak in the potential range between −0.9 and −0.7 V corresponds for the oxidation of the absorbed and adsorbed hydrogen, the peak from −0.6 to −0.4 V is for OH adsorption, and the peak at about −0.2 V can be ascribed to Pd oxide formation, respectively. In addition, the cathodic peak ranging from 0.0 to −0.4 V is due to the reduction of Pd oxide, and the peak between -0.6 to −0.8 V relates to the hydrogen adsorption/absorption40, 41. The reduction peak current density of PdO is 82 mA mg−1 for Pd/ZrO2-CeO2/C composite catalyst, which is significantly larger than other catalysts. This indicates the highest electrochemical activity of Pd/ZrO2-CeO2/C composite catalyst in present work.

Figure 4

Cyclic voltammograms of different catalysts in 1 M KOH solution at a scan rate of 50 mVs−1.

Figure 5 shows the cyclic voltammograms of different catalysts in 1 M KOH solution containing 1 M EG. There are two anodic peaks observed in the forward and reverse scans. The oxidation current increases with the potential increasing for EG oxidation in the forward scan, then decreases due to the reduced activity of Pd and CO poisoning43. The anodic peak appeared during the reverse scan could correspond to re-oxidation process of the intermediate product of EG17, 42. It is noticed that the current density (if) of forward anodic peak of Pd/ZrO2-CeO2/C (3700 mA mg−1) is much greater than that of Pd/C (1695 mA mg−1) and Pd/CeO2/C (2448 mA mg−1). This implies that the Pd/ZrO2-CeO2/C composite catalyst has highest catalytic activity for EG electro-oxidation. It has been reported that the positive shifts of Pd 3d5/2 peak of Pd-based catalysts indicates the decrease in the 3d electron density of Pd. The Pd with low 3d electron density is not easy to bind with the intermediate, and thus the intermediate coverage on Pd surface can be reduced43. Therefore, the highest catalytic activity of Pd/ZrO2-CeO2/C composite catalyst in present work can be attributed to the interaction between Pd and (Zr, Ce)O2 solid solution (in Figs. 2 and 3) as well as the smallest particle size of Pd (Fig. 1).

Figure 5

Cyclic voltammograms of different catalysts in 1 M KOH solution containing 1 M EG at a scan rate of 50 mV s−1.

Moreover, the chronoamperometry curves of different catalysts were collected in 1 M KOH containing 1 M EG as shown in Fig. 6. It is clear that the Pd/ZrO2-CeO2/C catalyst has a highest initial anodic oxidation current density because of its best electrocatalytic activity in EG. Moreover, there are rapid decays of the current densities observed for all catalysts, due to the formation of CO-like intermediates during EG oxidation13. Then the current decreases slowly and reaches a pseudo-steady state after 4000 s. It is worth noting that the Pd/ZrO2-CeO2/C composite catalyst exhibits a highest steady state current density during the EG oxidation measurement, indicating its best stability among all catalysts in present work. The current density of Pd/ZrO2-CeO2/C catalyst is about 1.7 times as that of Pd/CeO2/C catalyst (295.5 vs. 177.8 mA. mg−1) after 5000 s.

Figure 6

Chronoamperometric curves of different catalysts recorded at −0.25 V in 1 M KOH solution containing 1 M EG.

It is known that CO species are the main poisoning intermediate during the electro-oxidation process, thus a good catalyst for EG electro-oxidation should possess excellent CO electro-oxidizing ability. Figure 7 shows the CO-stripping voltammograms of different catalysts in 1 M KOH. It shows that the CO-striping onset potential of the Pd/ZrO2-CeO2/C composite catalyst is similar with all the catalysts studied, and only the peak areas are different, which is related to the electrochemical surface area.

Figure 7

CO-stripping voltammograms of different catalysts in 1 M KOH solution at a scan rate of 50 mV s−1.

Therefore, the electrochemical active surface area (EAS) is calculated by following equation44, 45


where Q is the charge for CO desorption electro-oxidation, m is the amount of Pd loaded, and C (420 μC cm−2) is the charge needed for the adsorption of a CO monolayer. It is obvious that the EAS of the Pd/ZrO2-CeO2/C catalyst is larger than that of Pd/C (117.9 vs. 101.1 m2 g−1), which further supports the promoted CO-stripping of (Zr, Ce)O2 solid solution. To clarify the catalytic effect of ZrO2-CeO2, the specific activity of catalysts has been calculated by normalizing the cyclic voltammograms results (in Fig. 5) to EAS result. It is also worth noting that the specific activity obviously increases from 1.68 mA cm−2 for Pd/C to 3.14 mA cm−2 for Pd/ZrO2-CeO2/C catalyst. Therefore, the inclusion of (Zr, Ce)O2 solid solution enhances the stability as well as activity of Pd/C catalyst, which could be related to the strong interaction between Pd and (Zr, Ce)O2 solid solution and the weaker adsorption strength between the Pd surface and CO as discussed for XPS result in Fig. 3.

The TEM images and particle size distribution of different catalysts after 900 cycles in the 1 M KOH solution containing 1 M EG are displayed in Fig. 8. It shows that the average diameter of Pd nanoparticles after 900 cycles increases to 6.5, 5.5, 4.9 and 4.5 nm for Pd/C, Pd/ZrO2/C, Pd/CeO2/C and Pd/ZrO2-CeO2/C, respectively. The smaller increasement in diameter of Pd particles for Pd/ZrO2-CeO2/C has been obtained compared with that of catalysts before test as shown in Fig. 1, which indicates its better stability in the alkaline solution. This result can be attributed to protective decoration of Pd/C by (Zr, Ce)O2 solid solution which can prevent Pd from dissolution and agglomeration during cycling46. It is also observed that the d-spacing of 0.227 which belongs to the (111) plane of cubic Pd, from the HRTEM images of all catalysts in Fig. 9e–h, and the corresponding d-spacing of ZrO2, CeO2 and ZrO2-CeO2 have been measured and confirmed, which is similar as the TEM analyses of the catalysts before cycling in Fig. 1.

Figure 8

TEM images of different catalysts after 900 cycles in the 1 M KOH solution containing 1 M EG, for (a) Pd/C, (b) Pd/ZrO2/C, (c) Pd/CeO2/C and (d) Pd/ZrO2-CeO2/C. Insets show the corresponding size distribution in (a,b,c) and (d), respectively. (e,f,g) and (h) are the HRTEM images for (a,b,c) and (d), respectively.

Figure 9

The relaxed (a) Pd4/CeO2 (111) and (b) Pd4/ZrO2-CeO2 (111) catalyst models used to study the CO absorption and desorption mechanism.


It is well established that the addition of oxides into Pd-based catalysts increases alcohol oxidation and the removal of adsorbed CO on the surface of catalysts. The higher catalytic activity of Pd/ZrO2-CeO2/C compared with that of Pd/CeO2/C in present work could be related to the addition of ZrO2 to CeO2. According to the bi-functional mechanism, the addition of ZrO2 probably more easily activates H2O to form oxygen-containing species (OHads) at lower potential. Then the CO-like intermediate species could be reacted with these oxygen-containing species on the surface of Pd surface to release the active sites for further alcohol oxidation30. It has also been reported that the synergistic effect can be obtained if intimate mixing (solid solution) is achieved, then the electrochemical properties could be modified47. Therefore, the improved electrocatalytic activity and stability of Pd/ZrO2-CeO2/C composite in present work can be mainly attributed to the strong interaction between Pd and (Zr, Ce)O2 solid solution as well as the synergistic effect between CeO2 and ZrO2.

First principle calculations were performed to further unravel the physical origin of the improved electrocatalytic activity and stability of Pd/ZrO2-CeO2/C composite. Since the CeO2 (111) surface is more stable than CeO2(110) surface48, we have proposed a catalyst model with 3 × 3 CeO2 p(111) surface slab and a Pd 4-atom cluster, referred to as Pd4/CeO2 (111) hereafter. According to our previously analysis, we have obtained (Zr, Ce)O2 solid solution with CeO2 structure by replacing 50% Ce atoms with Zr atoms. Herein, the special quasi-random structure (SQS) approach49 has been introduced to model the (Zr, Ce)O2 solid solution. Corresponding catalyst model refers to as Pd4/ZrO2-CeO2 (111) hereafter. Figure 9 illustrates the relaxed structures of Pd4/CeO2 (111) and Pd4/ZrO2-CeO2 (111) catalyst models. Very interestingly, the Pd cluster behaviors is very different on top of the CeO2 and (Zr, Ce)O2 solid solution surface. As can be seen in Fig. 9a, for the Pd4/CeO2 (111) catalyst model, the Pd atoms spread on top of the CeO2 surface, forming a 2D plane structure. On the other hand, the four Pd atoms gather into a tilted tetrahedron on top of the surface of (Zr, Ce)O2 solid solution, forming a 3D stereoscopic cluster in Fig. 9b. The corresponding charge transfer between the Pd4 cluster and oxide surface ρ chargetransfer illustrated in Fig. 8c and d are analyzed by:

$${\rho }_{{\rm{chargetransfer}}}={\rho }_{{{\rm{Pd}}}_{{\rm{4}}}}+{\rho }_{{\rm{Oxide}}}-{\rho }_{{\rm{catalyst}}}$$

where ρ Pd4, ρ Oxide and ρ catalyst are the self-consistent charge density of Pd4 clusters CeO2 (111) or ZrO2-CeO2 (111) surface, and Pd4/CeO2 (111) or Pd4/ZrO2-CeO2 (111) catalyst, respectively. As seen, the charge transfer between O and Pd atoms on the CeO2 (111) surface in Fig. 9c is stronger then on the ZrO2-CeO2 (111) surface, indicating that the chemical environment on the ZrO2-CeO2 (111) surface is more homogeneous. We performed the Bader charge50 analysis to quantify the transfer of charge density. The results show 0.592 e and 0.427 e net charge transferred from the Pd4 cluster to the CeO2 (111) and ZrO2-CeO2 (111) surface, respectively, indicating the 3D stereoscopic cluster is more stable than the 2D plane structure.

We assumed such structure difference leads to different anti-CO-poisoning properties. The required driving forces of CO desorption are evaluated by the following equation:


where E CO/catalyst shows the total energy of Pd4/CeO2 (111) or Pd4/ZrO2-CeO2 (111) catalyst with absorbed CO molecule, E catalyst corresponds to the total energy of Pd4/CeO2 (111) or Pd4/ZrO2-CeO2 (111) catalyst, and E CO is the total enegy of CO molecule. The corresponding CO desorption energies for the Pd4/CeO2 (111) and Pd4/ZrO2-CeO2 (111) catalyst are 2.759 eV and 1.836 eV. It is obviously that the desorption of the CO molecule from Pd4/ZrO2-CeO2 (111) catalyst is much easier than that from Pd4/CeO2 (111) catalyst. Hence, the Pd4/ZrO2-CeO2 (111) catalyst presents better anti-CO-poisoning properties, consistent with the best anti-CO-poisoning of the Pd/ZrO2-CeO2/C composite catalyst (in Fig. 7).

To further exploring the anti-CO-poisoning properties, the charge transfers from absorbed CO molecule to Pd cluster was studied by analyzing the charge density differences ρ diff, which is defined as:

$${\rho }_{{\rm{diff}}}={\rho }_{\mathrm{CO}/\mathrm{catalyst}}-({\rho }_{{\rm{catalyst}}}+{\rho }_{{\rm{CO}}})$$

where ρ Co/catalyst, ρ catalyst and ρ CO corresponding to the self-consistent charge density of Pd4/CeO2 (111) or Pd4/ZrO2-CeO2 (111) catalyst with absorbed CO molecule, Pd4/CeO2 (111) or Pd4/ZrO2-CeO2 (111) catalyst, and CO molecule, respectively. Figure 10 plots ρ diff for CO molecule absorbed on Pd4/CeO2 (111) and Pd4/ZrO2-CeO2 (111) catalyst. The violet isosurfaces present the charge depletion ρ diff < 0, while the cyan isosurfaces show the charge accumulation ρ diff > 0. As seen in Fig. 10a, the absorption of CO on top of the Pd4/CeO2 (111) catalyst will lead to charge depletion in the middle of the CO molecule and the Pd 2D flat cluster, which contributes to strong Pd-C bonding. Meanwhile, for the case of CO absorbed on the Pd4/ZrO2-CeO2 (111) catalyst as shown in Fig. 10b, the charge accumulation between the CO molecule and the Pd 3D stereoscopic cluster increases the repulsive force between the C and Pd atom, resulting in a weaker Pd-C bonding. Combining with our previously analysis, the 3D stereoscopic Pd cluster on (Zr, Ce)O2 solid solution contributes to the good anti-CO-poisoning properties of Pd4/ZrO2-CeO2 (111) catalyst.

Figure 10

Plots of charge density difference (violet: charge depletion, cyan: charge accumulation) for CO absorbed on top of the (a) Pd4/CeO2 (111) and (b) Pd4/ZrO2-CeO2 (111) catalysts.


In present work, the effect of (Zr, Ce)O2 solid solution on the structures and properties of Pd-based catalysts has been clearly demonstrated. The inclusion of (Zr, Ce)O2 solid solution reduces the particle size and increases the EAS of Pd nanoparticles, resulting in enhanced electrocatalytic activity of the composite catalyst for EG electro-oxidation in KOH solution. In addition, the strong interaction between Pd and (Zr, Ce)O2 solution decreases the Pd 3d electron density, which reduces the intermediate coverage on Pd surface and releases more active sites for EG electro-oxidation. The synergistic effect in (Zr, Ce)O2 also significantly increases the concentration of the OHads species on Pd surface and thus improves the stability and anti-CO-poisoning of Pd-based composite catalysts. Furthermore, the 3D stereoscopic Pd cluster on the surface of (Zr, Ce)O2 solid solution were explored based on first principle calculations, which leads to weaker Pd-C bonding and smaller CO desorption driving force. The findings on the good electrocatalytic properties of Pd/ZrO2-CeO2/C composite catalyst and the related mechanism will promote the development of stable catalyst for DAFCs application.


Sample preparation

26 mg of CeCl3·7H2O and 1 g urea (Sinopharm Chemical Reagent Co., Ltd, AR) were dissolved in 50 mL of deionized water. 84 mg Vulcan XC-72 carbon black was added into the solution, sonicated for 30 min and magnetic stirred for 1 h. The resulting solution was transferred into the oil bath at 90 °C for 3 h, washed with deionized water after cooling down naturally, and dried at 70 °C. The dried power was heated at 500 °C for 1 h in tube furnace under N2 atmosphere with a heating rate of 4 °C/min, then cooled down to get the support as CeO2/C. The ZrO2/C and ZrO2-CeO2/C were also prepared similarly. The molar ratio of ZrOCl2·8H2O (Sinopharm Chemical Reagent Co., Ltd, AR) to CeCl3·7H2O is 50:50 for preparing the ZrO2-CeO2/C. The mass ratio of the oxide to XC-72 carbon black is 1:7.

The catalysts were prepared through a borohydride reduction approach43, 51. 20 mg of PdCl2 (Shanghai Jiuyue Chemical Reagent Co., Ltd, AR) was sonicated in ultrapure water for 2 h. The prepared CeO2/C was sonicated in ultrapure water for 1 h. Two solutions were then mixed and stirred for 1 h, to obtain a solution with a nominal Pd-loading of 20 wt. %. The pH of this solution was adjusted to 9 using 1 M NaOH. NaBH4 was then added to the solution as a reduction agent, with a molar ratio of 1:8 for Pd and NaBH4. The resulting precipitate was filtered and washed with ultrapure water and ethanol, and then dried at 60 °C. The catalysts are designated as Pd/ZrO2/C, Pd/ZrO2-CeO2/C and Pd/CeO2/C, respectively. The Pd/C (Pd:C = 20:80 wt.%) was also prepared for comparison.

Materials characterizations

The high resolution transmission electron microscopy (HRTEM) measurement was conducted in an Electron Microscope system (Tecnai G2 F20 S-TWIN) at 200 kV. Samples were prepared by transferring the catalyst suspension to a copper grid. The catalysts after 900 cycles in 1 M KOH containing 1 M EG were also subjected to TEM measurement.

The electronic structures of Zr 3d and Ce 3d, in different species before and after Pd-loading, were investigated by X-ray photoelectron spectroscopy (ESCALAB 250, Thermo Scientific, Inc.) with a monochromatic Al Kα source (10 mA, 15 kV), respectively. The electronic structure of Pd 3d in different catalysts was also measured by XPS. The spectra were fitted by the Gaussian-Lorentzian method, with a background subtraction by Shirley’s method52.

Electrochemical measurements

3 mg of catalysts was added in 0.6 mL of Nafion solution (0.5 wt. %) and stirred for 30 min. 4 μL resulting ink was then transferred onto the electrode surface (glassy carbon disk, 3 mm in diameter), and dried at 70 °C for 10 min.

The electrochemical properties of catalysts were measured using an electrochemical workstation (CHI660D, Chenhua Inc., Shanghai, China) in a three-electrode system. The Pt plate (1 cm2) was served as the counter electrode, a Hg/HgO electrode for the reference electrode, and the glassy carbon disk electrode for the working electrode. All measurements were conducted in the water bath of 25 ± 1 °C. The measured Pd loading in the catalysts was 0.057 mg cm−2, by an inductively coupled plasma equipped with with atomic emission spectroscopy (ICP-AES).

The chronoamperometry was performed at a potential of −0.25 V (1 M KOH containing 1 M EG). In the electrochemical CO-stripping measurements, CO was bubbled into the solution for 15 min with a fixed the catalyst potential (0 V vs. Hg/HgO). The residual CO in the solution was removed by N2 (99.9%). The cyclic voltammograms (CVs) were conducted in the potential ranging from −0.9 V to 0.4 V vs. Hg/HgO with a sweep rate of 50 mV s−1 (1 M KOH and 1 M KOH containing 1 M EG).

First principle calculations

Our first principle calculations based on the density functional theory, were performed using the Vienna ab initio simulation package (VASP)53 in conjunction with the projector augmented wave (PAW) generalized gradient approximations (GGA)54 of Perdew-Burke-Ernzerhof (PBE)55 pseudopotentials. The valence electron configurations for C, O, Zr and Ce were 2s 22p 2, 2s 22p 4, 4s 24p 65s 24d 2 and 5s 25p 66s 24f 15d 1, respectively. The geometry convergence was achieved with the Γ symmetry K-point using the Gaussing smearing (σ = 0.02 eV) with the cut-off energy of 500 eV. The CeO2 p(111) surface slab is modeled by a (3 × 3) unit cell. The relaxation convergence for ions and electrons were 1 × 10−5 and 1 × 10−6 eV, respectively. The crystal structures and polyhedrons were visualized using the VESTA tool56.


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The authors gratefully acknowledge the financial support of the National Natural Science Foundation of China (Nos. 51301039, 51672045, 61622404 and 61504028), Key Program of University-industry Collaboration from Science and Technology Department of Fujian Province (No. 2015H6009), Shanghai Pujiang Talent Program (No. 15PJ1403300), Science and Technology Innovation Action Program from the Science and Technology Commission of Shanghai Municipality (No. 15520720200). They would also like to thank Xinqi Zhang for assistance with TEM/EDS and Zhenhuan Zheng for assistance with X-ray diffraction analysis.

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C.W. and Y.W. prepared the samples and tested the properties. B.S. performed the DFT calculations. D.T., T.Z. and C.C. designed the research. C.W., B.S. T.Z. and C.C. analyzed the data. All authors wrote the paper.

Correspondence to Baisheng Sa or Teng Zhang or Changxin Chen.

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