It is crucial to develop a catalyst made of earth-abundant elements highly active for a complete oxidation of methane at a relatively low temperature. NiCo2O4 consisting of earth-abundant elements which can completely oxidize methane in the temperature range of 350–550 °C. Being a cost-effective catalyst, NiCo2O4 exhibits activity higher than precious-metal-based catalysts. Here we report that the higher catalytic activity at the relatively low temperature results from the integration of nickel cations, cobalt cations and surface lattice oxygen atoms/oxygen vacancies at the atomic scale. In situ studies of complete oxidation of methane on NiCo2O4 and theoretical simulations show that methane dissociates to methyl on nickel cations and then couple with surface lattice oxygen atoms to form –CH3O with a following dehydrogenation to −CH2O; a following oxidative dehydrogenation forms CHO; CHO is transformed to product molecules through two different sub-pathways including dehydrogenation of OCHO and CO oxidation.
A complete oxidation of hydrocarbons has been a significant topic in the field of heterogeneous catalysis for decades since unburned hydrocarbons must be transformed in power plants or before release of gas exhaust from various engines of vehicles using gasoline, diesel, natural gas or liquid petroleum gas (a mixture of propane, isobutene, n-butane and ethane). Thermal stability of a catalyst (for removal of CH4 or other hydrocarbons) at a temperature of 1,300 °C for applications to power plants or at least 800 °C for engines using gasoline or diesel is requested. Ying et al. reported that CeO2 nanoparticles supported on barium hexaaluminate exhibits high activity at a quite high temperature and remains its structure up to 1,300 °C (ref. 1). Recently, Gorte, Fornasiero, and Farrauto and their coworkers reported that a catalyst of Pd nanoparticles caged in a porous CeO2 shell supported on Al2O3 exhibits exceptionally high activity for a complete oxidation of methane with a high thermal stability up to 850 °C (refs 2, 3). The activity of Co3−xCuxO4, Co3−xZnxO4, and Co3−xNixO4 for oxidation of hydrocarbons was reported in 1968 and the following studies4,5,6,7. A very recent study showed the high activity of these oxides in oxidation of (a) a mixture of liquefied petroleum gas and CO or (b) a liquefied petroleum gas without CO8.
Use of natural gas vehicles is a programme launched in Europe and other countries towards diversity of energy sources and utilization of methane, the inexpensive, earth-abundant energy sources9,10,11,12. The exhaust of natural gas engines has the following features9: low temperature (<500–550 °C), low CH4 concentration (about 1,000 p.p.m.), large amount of water vapour (10%), high O2:CH4 ratio, and presence of NOx or SOx (refs 9, 12). A complete oxidation of methane at a relatively low temperature (<500–550 °C) is critical for abating unburned methane of the exhaust of engines of natural gas vehicles9,11,12,13. Pt and Pd supported on Al2O3 are the well-studied catalysts9. Significant efforts have been made in fundamental understanding of mechanism of the complete oxidation of methane14 and optimization of catalytic performances of these Pt- or Pd-based catalysts9. From reaction mechanism point of view, Neurock and Iglesia et al. first elucidated the reaction mechanism on Pd-based catalysts at a molecular level14; these Pd-based catalysts exhibit different mechanisms of activation of C–H along increase of chemical potential of oxygen.
The high cost of precious metals has driven the search of catalysts made of earth-abundant elements. Spinel oxide, a type of reducible early transition metal oxides, consists of M2+ and M3+ in its lattice. Co3O4 is one of the spinel oxides. It has almost weakest M–O bonds among all transition metal oxides15,16. Oxygen vacancies can be readily generated even at a temperature below 25 °C (refs 17, 18). In addition, the barrier for hopping oxygen vacancies on the surface of Co3O4 is only 0.23 eV (ref. 17). Due to the high density of oxygen vacancies of surface of Co3O4 (refs 15, 19), Ni cations and oxygen vacancies are mixed at atomic scale, while Ni cations are integrated to the lattice of Co3O4 through formation of a doped spinel oxide NixCo3−xO4. Figure 1a schematically shows the integration of Ni cations, Co cations and surface lattice oxygen atoms and vacancies at atomic scale. Although catalytic activity of a complete oxidation of hydrocarbons on doped cobalt oxides was reported as early as 1968 (refs 4, 5, 6, 7, 8), there is lack of mechanistic understanding of the complete oxidation of hydrocarbons at a molecular level. Compared with the well-studied complete oxidation of CH4 on Pt or Pd-based catalysts9, the complete oxidation on NiCo2O4 could fellow a different mechanism.
Here we focus on mechanistic exploration of a complete oxidation of methane on NiCo2O4 at a molecular level. Multiple in situ techniques are used in experimental exploration of the catalytic mechanism. Surface chemistry of this mixed oxide during catalysis is tracked with ambient pressure X-ray photoelectron spectroscopy (AP-XPS)20. Vibrational signature of surface adsorbates is identified with in situ infrared spectroscopy. In addition, computational studies for understanding of the mechanism of the complete oxidation of methane on NiCo2O4 at a molecular scale are performed.
Catalytic performance for complete oxidation of CH4
Catalyst NiCo2O4 was synthesized with a coprecipitation method described in the section of Methods. X-ray diffraction (Fig. 1b) showed that NiCo2O4 nanoparticles have the same spinel structure as Co3O4. NiCo2O4 catalyst consists of nanoparticles with a size of 3–6 nm (transmission electron microscopic (TEM) images; Fig. 1c,d). With the same method, Ni0.75Co2.25O4 and Ni1.25Co1.75O4 were prepared. X-ray diffraction and TEM studies confirmed the formation of lattice of spinel oxide (Supplementary Figures 1 and 2, and Supplementary Methods).
Catalytic performances of a complete oxidation of CH4 on these catalysts were measured in a fixed-bed flow reactor. Certain amount of a catalyst given in figure captions was used in different experiments. 10% CH4 balanced with Ar, and 99.99% O2, and 99.99% Ar with certain flow rates were mixed and then flowed through a catalyst bed. The molar ratio of the introduced CH4 and O2 is 1:5 for all experiments in Fig. 2. NiCo2O4 is extraordinarily active in combustion of CH4 to CO2 and H2O. CH4 is completely combusted at 350 °C, while gas hourly space velocity (GHSV) of methane is 24,000 ml 5% CH4 g−1 h−1 (Fig. 2). At the same GHSV, pure Co3O4 and pure commercial NiO with surface areas similar to NiCo2O4 exhibit a conversion of only 8% and 0% at 350 °C, respectively (Fig. 2). The pure Co3O4 without any Ni cations exhibits a much lower conversion than NiCo2O4 though it has the same lattice of a spinel structure. This distinct difference in catalytic performance between NiCo2O4 and pure Co3O4 in the temperature range of 200–425 °C shows that Ni cations are crucial sites for dissociation of CH4, which was supported by experimental studies and theoretical findings in the following sections. The catalytic performance of complete combustion at 350 °C is remained even after heating to 550 °C and then cooling to 200 °C (Fig. 3a). Kinetic studies were performed in the temperature range of 270–330 °C, while catalysis was in a kinetics control regime by controlling conversions <10%. The measured activation barrier is about 108 kJ mol−1 (Supplementary Fig. 3). In addition, NiCo2O4 exhibits durability in complete oxidation of methane at 350 °C and 550 °C for over 48 h (Fig. 3b,c). The thermal stability of catalyst structure was confirmed by the preservation of X-ray diffraction pattern of NiCo2O4 after a complete oxidation at 550 °C (Supplementary Fig. 4). In addition, NiCo2O4 remains the original particle size after a complete oxidation at 550 °C as shown in Supplementary Fig. 5. This is consistent with the thermal stability of NiCo2O4 suggested by the thermal analysis of coprecipitated products and NiCo2O4 (ref. 21).
Surface chemistry of NiCo2O4 during catalysis
Measurements of bulk composition of NiCo2O4 catalyst using inductively coupled plasma Auger electron spectroscopy show that atomic ratio of Ni and Co in bulk of the NiCo2O4 nanoparticles is 1:2. Similar to the obvious difference in composition of bimetallic nanoparticle between surface and bulk22, the difference in atomic ratio of Ni/Co of NiCo2O4 catalyst between surface and bulk was uncovered here as well.
To achieve a deep understanding of the complete oxidation of methane on NiCo2O4, we performed in situ studies using AP-XPS15,20,23,24 in the temperature range of 60–400 °C by following the reaction conditions used for measurements of catalytic performances in a fixed-bed flow reactor. Surface chemistry of NiCo2O4 (a) in UHV, (b) in a reactant gas (CH4 or O2) at room temperature, (c) in a mixture of reactant gases (CH4+O2) at room temperature and (d) in a mixture of reactant gases (CH4+O2) in the temperature range of 25–400 °C were studied. Photoemission features of Co 2p, Ni 2p, and O 1s of NiCo2O4 collected under conditions (a), (b) and (c) are quite similar; in addition, the atomic ratios of O/(Ni+Co) of the catalyst surface under the three conditions are the same. However, the atomic ratio O/(Ni+Co) in the gaseous environment of CH4 and O2 exhibits a temperature-dependent evolution which will be discussed in the following paragraphs.
During the data acquisition of in situ studies, NiCo2O4 catalyst was remained in a mixture of CH4 and O2 (molar ratio 1:5) in Torr pressure range. Figure 4, Supplementary Fig. 6 and Supplementary Fig. 7 present photoemission features of NiCo2O4, Ni0.75Co2.25O4 and Ni1.25Co1.75O4 during catalysis, respectively. As shown in Fig. 4a,b, the photoemission features of Ni 2p and Co 2p remain constant in the temperature ranges of 60–400 °C. Surprisingly, two C 1s peaks at 285.6 eV (peak 1) and 288.3 (peak 2) were clearly observed even at 60 °C (Fig. 4d). Figure 5a shows the evolution of the surface atomic ratio, of the two C 1s peaks of Fig. 4d along the increase of catalysis temperature. One interesting evolution is a quick increase of species 2 (peak 2 in Fig. 4d), a following decrease, and then a nearly complete disappearance of this species at about 250 °C (red lines in Fig. 5a,b) where the conversion of CH4 starts to increase largely (Fig. 2). The sharp decrease of on NiCo2O4 (red line in Fig. 5a) and a following decrease and then disappearance at 250–300 °C along the rapid increase of catalytic conversion at 250–300 °C (green line in Fig. 2) suggests species 2 (peak 2 in Fig. 4d) is an intermediate in the formation of CO2 molecules.
In situ infrared studies of catalysts helped assign the two species corresponding to peaks 1 and 2 in Fig. 4d. As shown in Fig. 6, vibrational peaks at 1,280 1,430 and 1,561 cm−1 were observed in the temperature range of 50–160 °C. Referred to the literature25, these vibrational signatures are contributed from formate species (OCHO). The assignment of these vibrational peaks to a formate species is supported by the agreement between C 1s photoemission peak at 288.3 eV (peak 2 in Fig. 4d) and 288.5 eV of the reported formate species25. Thus, both in situ photoemission feature of C 1s and in situ vibrational signature of surface species suggest the formation of OCHO species on the surface at a relatively low temperature. C–H vibrational peaks at 2,900–3,000 cm−1 were identified during in situ studies of CH4 combustion on NiCo2O4. They are contributed from C–H stretching of the spectator CHn species formed from dissociative adsorption of CH4, supported by the low C 1s binding energy of CHn (peak 1) at 285.9–284.8 eV (refs 25, 26, 27), and C–H stretching of the intermediate OCHO.
To investigate whether that the C 1s photoemission feature at 284.9–285.8 eV (peak 1 in Fig. 4d) is assigned to adsorbed CHn species or accumulated atomic carbon of coke, surface of the active catalyst at 400 °C or 140–200 °C in the mixture of CH4 and O2 (1:5) was tracked on CH4 was purged but O2 kept. The in situ AP-XPS (Supplementary Fig. 8) suggests that the left CHn species on surface at 400 °C reacted with oxygen upon CH4 was purged and but O2 remained. As shown in Supplementary Fig. 8, C 1s photoemission feature of the left CHn species disappeared within a few minutes due to a quick oxidation by O2 to form CO2. A similar study was designed to test whether the peak 1 of C 1s spectrum observed at 150 °C in the mixture of CH4 and O2 (1:5) (Fig. 4d) is coke-like carbon or chemisorbed CHn species. As shown in Supplementary Fig. 9, these carbon-containing species formed at 140 °C reacted with O2 to form CO2 and disappeared at 200 °C in O2. Therefore, these designed experiments (Supplementary Figs 8 and 9) suggest that the C1s at 284.9–285.8 eV (peak 1) is not contributed from accumulated coke-like carbon since a coke-like carbon is not readily oxidized to CO2 at 400 °C or 140–200 °C (ref. 28). Therefore, both C 1s photoemission feature and C–H vibrational signatures allow us for assigning the carbon-containing species of peak 1 in Fig. 4d to CHn species. It is noted that the coke-like carbon does form by dissociation of CH4 when NiCo2O4 catalyst is kept in pure CH4 (Supplementary Fig. 10d); in addition, without O2, nickel cations of NiCo2O4 are reduced to metallic state at 400 °C (Supplementary Fig. 10a); along this reduction, coke-like carbon are formed at 400 °C (Supplementary Fig. 10d). It suggests a strong binding of coke-like carbon on metallic Ni atoms28. By introducing O2 to the surface of carbon layers at 400 °C, the C 1s photoemission feature of coke-like carbon still remains. It further suggests the nature of coke-like carbon formed on NiCo2O4 in the lack of molecular O2. By introducing the mixture of CH4 and O2 (1:5) to this surface covered with a layer of coke, there is no conversion of CH4 anymore on it since the catalyst surface has been coved with coke-like carbon.
Figure 7a presents the evolution of the surface atomic ratio, along the increase of catalysis temperature of NiCo2O4. There are two processes involved in the evolution of atom ratio. The formation of OCHO species with a following desorption of CO2 generates surface oxygen vacancies; an opposite process is the filling of oxygen vacancies with oxygen atoms through dissociation of molecular O2. The ‘U’ shape evolution of atomic ratio shows that more oxygen vacancies are created at a medium temperature (150–250 °C). The decrease of the ratio, (namely, the increase of density of oxygen vacancies) at ≤250 °C likely suggests that the formation of oxygen vacancies through desorption of product molecules is relatively faster than filling oxygen vacancies through dissociation of O2 in this temperature range. At a relatively high temperature such as 300 °C, the atomic ratio starts to increase. It probably results from the accelerated dissociation of O2 and thus a faster refilling of surface oxygen vacancies (at a higher temperature) than consumption of oxygen atoms through transforming the OCHO intermediate to product molecules CO2. The turning point of ratio (about 250 °C) suggests that there is a barrier for O2 dissociation. For a temperature ≤250 °C, the filling of oxygen vacancies through dissociation of molecular O2 on oxygen vacancies is kinetically slower than the creation of oxygen vacancies through desorption of intermediate or product molecules; thus, the net outcome is the decrease of ratio at a relatively low temperature. At a relatively high temperature (≥250 °C), however, dissociation of O2 is accelerated and thus oxygen vacancies are filled rapidly; therefore, the overall consequence is the increase of surface lattice oxygen at a temperature ≥250 °C. Alternatively, a potential oxygen-containing spectator could possibly be formed. It may contribute to the increase of O/(Ni+Co) ratio. Very similar ‘U-shape’ evolution of atomic ratio was observed on Ni0.75Co2.25O4 and Ni1.25Co1.75O4 (Fig. 7b,c) along the increase of the catalysis temperature of complete oxidation of methane.
In situ studies using isotope-labelled reactant and catalyst
Both in situ AP-XPS and infrared studies have shown the formation of the two species on NiCo2O4 surface in the mixture of CH4 and O2, formate (species 2) and CHn (n=0–3; species 1). To elucidate the source of oxygen atoms of the intermediate of OCHO species, we performed two temperature programmed reactions using isotope-labelled reactant and isotope-labeled catalyst: (1) CH4 and on (Fig. 8a) and (2) CH4 and on an isotope-labeled catalyst () (Fig. 8b).
In the complete oxidation of CH4 in on (Fig. 8a), products formed in the reaction cell of the AP-XPS were measured with an on-line mass spectrometer. One of the products, CO16O18 (M/z=46; green line in Fig. 8a) was clearly observed. The formation of CO16O18 suggests that surface lattice oxygen atoms O16 of participated into the formation of CO2 since the reactant gas does not have O16 atoms. The co-existence of O16 and O18 in CO16O18 product suggests that molecular O2 dissociates on surface during complete oxidation of CH4.
Another experiment is the CH4 combustion in on an isotope-labeled catalyst (Fig. 8b). The isotope-labeled catalyst was prepared by annealing the catalyst to 350 °C in a flowing . The preparation of was done in an attached high-pressure reactor of AP-XPS system which is different from the reaction cell of AP-XPS since our AP-XPS system has both reaction cell for AP-XPS studies and high-pressure reactor for pretreatment. Upon the preparation, was purged and a UHV environment (3 × 10−9 torr) was achieved before was transformed to the reaction cell of AP-XPS. Then, combustion of CH4 was performed on this isotope-labeled catalyst in pure in the reaction cell of AP-XPS. The evolution of partial pressure of the three potential products CO16O16 (M/z=44), CO16O18 (M/z=46), and CO18O18 (M/z=48) were recorded with the mass spectrometer (Fig. 8b). It is noted that CO16O18 (M/z=46) was produced even at a relatively low temperature 130–150 °C; However, the partial pressure of CO16O18 (M/z=46) decreased to its base line at a temperature higher than 150 °C. The decrease of CO16O18 partial pressure results from that fact that the source of O18 atoms in the isotope-labelled catalyst is limited. The observation of CO16O18 shows that the surface lattice oxygen atoms directly participate into the formation of intermediate towards formation of product molecules.
Catalytic performance for removal of CH4 in gas exhaust
To examine the catalytic performance of NiCo2O4 in a complete oxidation of CH4 of gas exhaust of an engine of natural gas, we measured catalytic performance of a complete oxidation of CH4 on NiCo2O4 in two different mixtures with gas compositions (Fig. 9) similar to the exhaust of lean-burn natural gas engine: (1) CH4 0.2%, O2 5%, CO2 15%, H2O 10% balanced with Ar with a flow rate of 200 ml min−1 (Figs 9a), and (2) CH4 0.2%, O2 5%, NO 0.15%, H2O 10% balanced with Ar (Fig. 9b). These gas compositions are typically used in the evaluation of catalytic performance of Pd- and Pt-based catalysts for a complete oxidation of CH4 in the exhaust of engines of natural gas11,12,13. In the mixture of CH4 0.2%, O2 5%, CO2 15% and H2O 10%, balanced with Ar, CH4 can be completely oxidized to CO2 and H2O on 200 mg NiCo2O4 at 425 °C (Fig. 9a). Compared with 200 mg of NiCo2O4, 200 mg of 2.2wt%Pd/Al2O3 can completely oxidize the mixture of 0.2% CH4, O2 5%, CO2 15% and H2O 10% at 500 °C or higher11. Thus, NiCo2O4 exhibits higher activity than Pd/Al2O3 in the complete oxidation of CH4 of exhaust gas in the temperature range of 400–500 °C. In the case of CH4 0.2%, O2 5%, NO 0.15% and H2O 10% balanced with Ar, CH4 can be oxidized completely to CO2 and H2O at 475 °C, while 200 mg NiCo2O4 is used (Fig. 9b). As the cost of Pd per kg is largely higher than nickel oxide and cobalt oxide by >3,000 times, the cost of raw materials of NiCo2O4 is <1% of the catalyst 2.2wt%Pd/Al2O3. Thus, NiCo2O4 is more active and certainly cost-effective compared with Pd/Al2O3 or Pt/Al2O3.
The NiCo2O4 crystal structure was built by substituting Ni with Co in Co3O4 crystal structure. As shown in Fig. 10, three different substitution models of crystals were tested in our calculations, namely substituting two Co3+ with two Ni3+ (type I, Fig. 10a), substituting one Co3+ and one Co2+ with one Ni3+ and one Ni2+, respectively (type II, Fig. 10b ), and two Co2+ with two Ni2+ (type III, Fig. 10c). The type I crystal structure was found to be the most stable in our calculations, while the type II was slightly less stable by 0.01 eV per unit cell higher in energy. The type III was most unfavourable thermodynamically, 0.20 eV higher per unit cell than that of type I. In the following calculations, types I and II were considered.
Stabilities of different facets
Four different surfaces namely NiCo2O4(100), NiCo2O4(110)-A, NiCo2O4(110)-B and NiCo2O4(111), were chosen for both type I and type II crystals based on the X-ray diffraction results and our previous work on Co3O4 (ref. 29). The optimized structures were shown in Supplementary Fig. 11 and Supplementary Fig. 12. The surface energies of all the eight surfaces were listed in Supplementary Table 1. For both type I and type II crystals, (110)-A and (110)-B surfaces exhibit slightly higher surface energies by 0.02 or 0.03 eV than (100). (110)-A, (110)-B, and (100) of types I and II crystals with relatively low surface energies were considered in the following studies of surface reactivities.
Reactivities of different facets
To examine the reactivities of (110)-A, (110)-B, and (100) of type I and II crystals, the dissociations of the first C–H of CH4 on these surfaces were investigated. Activation energies of these dissociations were listed in Supplementary Table 2. Transition states for these dissociations were presented in Supplementary Fig. 13 and Supplementary Fig. 14. These calculations (Supplementary Table 2) suggest that the 110-B of type I crystal are the most active for CH4 activation on Ni3+ with lowest activation energy of only 0.52 eV which is lower than those on Ni(111) (0.88 eV)30, Ni(211) (0.61 eV)30 and Pd(100) (0.79 eV)31. Therefore, the low barrier on 110-B of type I crystal is responsible for the high reactivity of NiCo2O4 catalyst.
Active sites for dissociation of the first C–H of CH4
To assign the sites for dissociation of CH4 to CH3, the binding strengths of CH3 on cobalt and nickel sites of NiCo2O4(110)-B surfaces of both type I and type II crystals were calculated (Supplementary Table 3). The adsorption energies of CH3 on nickel sites of (110)-B are stronger than those on cobalt sites for both types of crystals. In addition, as shown in Supplementary Table 2 the activation barrier for dissociation of CH4 to CH3 on Ni3+ of the most active surface NiCo2O4 (110-B) of crystal type I is much lower than Co3+ of this surface.
These DFT calculations suggest that Ni3+ cations are the sites for activating the first C–H of CH4. This is consistent with experimental observation. In situ studies of Ni0.75Co2.25O4−x and Ni1.25Co1.75O4−x with AP-XPS were performed under the same catalytic condition as NiCo2O4−x. In these parallel experiments, the atomic fraction of Ni cations to the total of Ni and Co cations on the catalyst surface during catalysis was measured. As shown in Supplementary Fig. 15, the actual fractions of Ni cations on surfaces of Ni0.75Co2.25O4−x, NiCo2O4−x, and Ni1.25Co1.75O4−x are 0.33, 0.51 and 0.44 at 250 °C, respectively. The conversions on Ni0.75Co2.25O4−x, Ni1Co2O4−x, and Ni1.25Co1.75O4−x at 275 °C are 10%, 27% and 17% (Supplementary Figure 16), respectively. The correlation between atomic fractions of Ni cations in Supplementary Fig. 15 and the catalytic conversion presented in Supplementary Fig. 16 shows that a higher atomic fraction of Ni cations on surface of a NixCo3−xO4 catalyst offers higher conversion of CH4. It further suggests that Ni cations instead of Co cations are active sites for activating C–H of CH4.
Mechanism of complete oxidation of CH4 on NiCo2O4
To fully understand the mechanism of CH4 complete oxidation on NiCo2O4, a systematic investigation of potential reaction pathways was carried out on the most active surface, (110-B) of type I crystal of NiCo2O4. After the dissociation of CH4 to CH3, there are two different possibilities for the next elementary steps: a further dissociation of CH3 into CH2 (called dehydrogenation in Supplementary Fig. 17) or a coupling of carbon atom of CH3 with oxygen atom of surface lattice (called oxidation in Supplementary Fig. 17). In order to determine which step is more favourable, we calculated the activation energies and enthalpy change for the two potential steps. The calculated energy profiles and the corresponding geometries were shown in Supplementary Fig. 17. Upon the first C–H dissociation, CH3 species is oxidized into CH3O binding to a Ni cation. The thermodynamically and kinetically favourable oxidation step forms an intermediate, CH3O. This is different from the continuous dehydrogenation of CH3 on Pd surface14. This preference of oxidation to CH3O instead of further dehydrogenation to CH2 or CH species could be understood as follows: the low coordinated species, such as CH2 or CH, need more than one binding sites to stabilize them; however the singly dispersed nickel cations on surface lattice of Co3O4 are not an adsorption site consisting of continuously packed Ni atoms for CH2 or CH. Therefore, a further dehydrogenation of CH3 to CH2 to CH is a high endothermic step on NiCo2O4 compared with the pathway of oxidation.
Supplementary Figure 18 presents the two potential reaction pathways A and B after the formation of CH3O species. DFT calculations show that pathway B is the preferred one. The following section will describe this preferred pathway. On the basis of the experimental results and previous calculations29,32, CHO species plays very important roles in the oxidation of methane on many different catalyst surfaces; thus CH3O could dehydrogenate to CH2O and then CHO with a following oxidation to form product molecules.
For dehydrogenation of CH3O to CHO, there are two different dehydrogenation pathways schematically shown in Supplementary Fig. 18: (i) the dehydrogenation of CH3O by the OH species of nickel site (pathway A shown in red in Supplementary Fig. 18); (ii) the dehydrogenation by the O species of nearby cobalt site (pathway B shown in black in Supplementary Fig. 18). On the basis of the energy profiles of the two pathways in Supplementary Fig. 19a, pathway B is more favourable than pathway A, which suggests that the dehydrogenation of CH3O by oxygen atoms (not shown) bonded to nearby cobalt site (pathway B) is preferred over a dehydrogenation of CH3O by OH species bonded to nickel site (Supplementary Fig. 18) in the overall reaction (pathway A).
Transformation of intermediate CHO to product molecules
As mentioned above, the transformation of intermediate CHO to product molecules could go through a sub-pathway of OCHO dehydrogenation (marked with purple in the right panel of Supplementary Fig. 18) other than the sub-pathway of CO oxidation (marked with black in the right panel of Supplementary Fig. 18). Supplementary Figure 21a shows the two sub-pathways considered in our DFT calculations. Our DFT calculations revealed that each sub-pathway includes two steps with two transition states and one intermediate. OCHO is the intermediate of the sub-pathway of OCHO dehydrogenation (Supplementary Fig. 21).
In the sub-pathway of OCHO dehydrogenation (red in Supplementary Fig. 21a,b), the CHO couples with oxygen atom and thus forms an intermediate OCHO (the first step in transforming CHO to product molecules); then the intermediate OCHO is dehydrogenated to CO2 (the second step); it is quite different from the sub-pathway of CO oxidation (black line in Supplementary Fig. 21a,b). We calculated the sub-pathway of OCHO dehydrogenation for transforming CHO to product molecules. The calculated energy profiles of the two sub-pathways were presented in Supplementary Fig. 21b. The geometries of transition states and intermediates of the sub-pathways of OCHO dehydrogenation and CO oxidation were presented in Supplementary Fig. 21c and Supplementary Fig. 21d, respectively.
From the calculated energy profiles presented in Supplementary Fig. 21b, several interesting features were found. The barrier of the first transition state in the sub-pathway of OHCO dehydrogenation (red line in Supplementary Fig. 21b) is lower than that of the first barrier in the sub-pathway of CO oxidation (black line in Supplementary Fig. 21b); in addition, the OCHO intermediate in the sub-pathway of OCHO dehydrogenation is more thermodynamically stable than the intermediate of the sub-pathway of CO oxidation by 0.63 eV. Thus, the formation of OCHO intermediate is thermodynamically and kinetically favourable. However, the barrier for transforming OCHO intermediate to CO2 is higher than the second barrier of the sub-pathway of CO oxidation (Supplementary Fig. 21b). Therefore, the formed OCHO intermediate could be experimentally observed at a relatively low temperature. In fact, our in situ studies of the catalyst surface in the mixture of CH4 and O2 with AP-XPS did identify the intermediate OCHO at a temperature lower than 200 °C; the C 1s photoemission feature of this intermediate is at 288.3 eV which is consistent with the OCHO species reported in literature25. In addition, the observed vibration signatures of this intermediate at 1,280, 1,430, and 1,561 cm−1 in situ infrared studies (Fig. 6) at 160 °C are consistent with the OCHO species formed in water–gas shift.25
In the sub-pathway of OCHO dehydrogenation, the second step (from OCHO intermediate to product molecules shown in red line in Supplementary Fig. 21b) is highly exothermic with a free energy change of −3.50 eV. Therefore, at high temperature the OCHO intermediate can readily overcome the barrier and transform to product molecule CO2, driven by the thermodynamics factor although the barrier of the second transition state is relatively high compared with the second one in the sub-pathway of CO oxidation. In fact, the evolution of C 1s photoemission feature at 288.3 eV during catalysis from low temperature to high temperature shows that this intermediate OCHO disappears at about 200 °C along the increase of catalysis temperature (Fig. 4d).
In situ studies using ambient pressure photoelectron spectroscopy, vibrational spectroscopy, and isotope-labelled experiments show that (1) molecular O2 dissociates on surface oxygen vacancies; (2) the dissociated oxygen atoms fill in oxygen vacancies and couple with hydrogen atoms dissociated from intermediate to from OH and then H2O molecules; (3) CH4 dissociates on Ni cations to form CH3 with a following oxidation to CH3O; (4) intermediate CHO is formed through dehydrogenation of CH3O with oxygen species of nearby cobalt site; (5) CHO is transformed to CO2 and H2O through two sub-pathways termed OCHO dehydrogenation and CO oxidation. Due to high activity and low cost of NiCo2O4 catalyst in completely oxidizing CH4 to CO2 and H2O at a relatively low temperature, NiCo2O4 is a very promising catalyst for removing CH4 of gas exhaust of natural gas engine through a complete oxidation.
The mechanisms of methane oxidation on NiCo2O4(100)-B are different from those on metal surfaces14,30,32. For instance, CH4 on metal surfaces sequentially and continuously dehydrogenates to CH species and then is oxidized to an intermediate CHO, while our studies suggest that after dissociation of first C–H in methane, the CH3 species will couple with oxygen atom of the lattice oxygen, forming CH3O species. The lack of direct dehydrogenation of CH3 to CH2 and then to CH on NiCo2O4 likely results from the low binding energy of CH2 or CH species on isolated Ni cations anchored on surface lattice of Co3O4. In other words, the separated Ni cation sites could not stabilize the low coordinate species such as CH2 and CH. In these calculated pathways on the NiCo2O4(100)-B, the surface lattice oxygen atom in the nearby cobalt sites was found to be very important in the dehydrogenation of CH3O.
Computational studies suggest that the pathways from transferring CHO to CO2 are different from that on metal surface14,33,34. Sub-pathway of CO oxidation and sub-pathway of OCHO dehydrogenation were both proposed for the transformation of CHO intermediate to CO2. CO oxidation sub-pathway was found more kinetically favourable in the second elemental step (Supplementary Fig. 21b). Furthermore, the OCHO intermediate (red in Supplementary Fig. 21) was found to be stable at low temperature due to the high activation barrier (1.64 eV) for transforming the intermediate OCHO to product molecules. However, this intermediate (OCHO) is unstable at high temperature due to the exothermic nature of the transformation from OCHO intermediate to CO2 (Supplementary Fig. 21b). Compared to the intermediate of the sub-pathway of CO oxidation, the higher thermodynamic stability of OCHO intermediate of the sub-pathway of OCHO dehydrogenation and its kinetically unfavourable transformation to CO2 make it observable at a relatively low temperature.
NiCo2O4, Ni1.25Co1.75O4 and Ni0.75Co2.25O4 nanoparticles were all synthesized through a co-deposition precipitation and a following thermal decomposition. The chemicals Co(NO3)2·6H2O (≥98%), Ni(NO3)2·6H2O (≥97%), and KOH (≥85%) were purchased from Sigma-Aldrich and were used as received. 0.01 mol Ni(NO3)2·6H2O, and 0.02 mol Co(NO3)2·6H2O were physically mixed and completely dissolved in 50 ml deionized water. Then 150 ml KOH (1 M) was added under the bubbling of N2 and with continuously stirring. During this process the temperature was kept at room temperature. A blue colloidal solution was obtained after the introduction of KOH. A dark blue precipitate was collected on centrifuging the prepared solution. Then, the dark blue precipitate was first washed with hot deionized water (60 °C) for several times with a following drying at 130 °C for 24 h. The obtained black solid was grounded to powder and was further calcined at 350 °C in air for 24 h, forming the as-synthesized catalyst NiCo2O4. To synthesize Ni0.75Co2.25O4 and Ni1.25Co1.75O4, the method is almost the same as the one for the synthesis of NiCo2O4. For synthesis of Ni1.25Co1.75O4, 0.0125, mol Ni(NO3)2·6H2O, and 0.0175, mol Co(NO3)2·6H2O were used. 0.0075, mol Ni(NO3)2·6H2O and 0.0225, mol Co(NO3)2·6H2O were used for the synthesis of Ni0.75Co2.25O4.
Powder X-ray diffraction patterns of NiCo2O4, Ni1.25Co1.75O4, and Ni0.75Co2.25O4 nanocatalysts were collected on a Bruker D8 advance XRD using nickel-filtered Cu Kα radiation (λ=1.54056 Å). The measurements were operated at 40 kV and 40 mA in a continuous mode with the scanning rate of 4.2° min−1 in the 2θ range from 10° to 80°.
The size, shape and lattice fringe of catalysts were identified by high-resolution transmission electron microscope (FEI, Titan 80−300) operated at an accelerating voltage of 200 kV or lower. Image analysis was performed with Digital Micrograph (Gatan) software. The catalyst samples for TEM characterization were prepared by dropping their colloidal solutions onto copper grids supported on carbon films.
In situ studies of catalysts under reaction conditions and during catalysis
The in situ characterizations of surface chemistry of NiCo2O4, Ni0.75Co2.25O4, and Ni1.25Co1.75O4 nanocatalysts during catalysis were performed on the in-house AP-XPS system. Monochromated Al Kα line was used as X-ray source. Unlike traditional UHV studies, in AP-XPS studies reactant gases are introduced to continuously flow through the catalyst at a desired temperature in the reaction cell while data acquisition is going on. Thus, the in situ study is defined to be a study in which the measurement of catalyst surface or adsorbate is being performed, while a catalyst is buried in gas reactant (s). The in situ characterization of AP-XPS22,35,36 could be different from the in situ studies defined in other places since sometimes in situ study is defined as a characterization of a sample without changing location/position after a sample preparation or vapour deposition.
The reaction cell was incorporated into the UHV chamber of AP-XPS system. Gas flows through the cell and exits through the exit port and an aperture that interfaces the gaseous environment in the reaction cell and vacuum environment of the prelens. Flow rate in the reaction cell was measured through a mass flow metre installed before the entrance of the reaction cell. In this study, the typical flow rate of pure gas is in the range of 3–5 ml min−1. As the gas source used in AP-XPS studies is pure gas, 3–5 ml min−1 equals to 60–100 ml min−1 of 5% reactant gas used in catalytic measurements in a fixed-bed flow reactor. The total pressure of the mixture gas at the entrance is measured with a capacitance gauge, while the pressure at the exit is measured with another capacitance gauge. An average of the pressures at entrance and exit is defined to be the pressure above the catalyst in the reaction cell. An external heating source in the UHV environment heats the catalyst in the environment of reactant gases in the reaction cell. More detailed description of the in-house AP-XPS system can be found in our previous publications20.
To avoid surface charging, we use Au, Ag, or HOPG to load catalysts for AP-XPS studies and control the thickness of catalyst layer on a surface19,37,38. In this work, we use Au foil as the substrate to physically load a thin layer of nanocatalysts. The Au foil is deliberately roughened using a SiC knife to increase the adhesion for loading. The apparent binding energies of Au 4f, Ni 2p, Co 2p, and O 1s of sample prepared on the Au substrate are very close to their real values, suggesting there is no identifiable surface charging. All XPS spectra are calibrated to their corresponding Au 4f7/2 binding energy which is at 84.0 eV. Analyses of XPS peaks are performed with Casa XPS program.
In situ infrared studies are performed in a reaction cell filled with 1 bar reactant gas at Oak Ridge National Lab. This reaction cell can be heated up to high temperatures. The same catalytic condition as measurements of catalytic performances was used in the infrared studies.
On-line observation of products at different temperatures
Our in-house AP-XPS system also allows us to monitor the change of the gas composition during catalysis with a quadrupole mass spectrometer. Three differential pumping stages were installed between the reaction cell and the energy analyser. The aperture mounted on the reaction cell separates the high-pressure environment of the reaction cell from the vacuum of the first differential pumping stage (prelens), and also allows for leaking gases on the reaction cell into the differential pumping stages. The analyses of gas composition at different temperatures during catalysis were done by a quadrupole mass spectrometer, which is mounted at the second differential pumping stage of the AP-XPS system. To exclude the possibility that gas expansion at a high temperature or fast diffusion of molecules from reaction cell of AP-XPS to UHV chamber of mass spectrometer results in an increase of partial pressure of product molecules, Ar gas was introduced as a reference gas (background) to the reaction cell. No change in the partial pressure of Ar along with the increase of temperature of catalysts shows that the increase of partial pressure of CO2 and H2O is not due to thermal expansion of gas at a relatively high temperature.
Such an on-line analysis of gas composition (reactants and products) in the reaction cell of AP-XPS allows for building a simultaneous correlation between the products and real-time surface chemistry of catalysts at different catalysis temperatures. The on-line mass spectroscopy experiments allow for tracking evolution of different products at different temperatures formed through isotope-labeled catalysts or through using isotope-labelled reactant during data acquisition of in-situ AP-XPS studies.
Measurements of catalytic performance
The catalytic performance was measured in a fixed-bed tubular quartz micro flow reactor (inner diameter=6 mm, length=300 mm), at atmospheric pressure. The catalyst (25–500 mg) was sieved (40–60 mesh) and loaded into the reactor between two layers of quartz sands, packed in between two quartz wool plugs. The catalyst was heated in a furnace equipped with a proportional-integral-derivative temperature controller. The temperature of the catalyst was measured with a K-type thermocouple inserted into the reactor and touching the catalyst bed.
The reactant gas composition was controlled by varying the flow rates of CH4 mixture (10% CH4 balanced in Ar) and O2 (pure O2). The flow rate of CH4 mixture (10% balanced in Ar) and O2 (pure) was precisely controlled through their own mass flow metres (Dakota Instruments, Inc.). When vary the flow rate of CH4 mixture and O2, the ratio of pure CH4 to pure O2 was always keeping at 1:5. The typical flow rate of CH4 mixture (10% balanced in Ar) is 100 ml min−1, while the flow rate of O2 (pure) is 50 ml min−1. The reliability of the fix-bed reactor was checked through a blank experiment with the same experimental parameters including reactant gases, flow rate and reaction temperature. In the blank experiment, only silica supporting material was loaded in the reactor. No appreciable conversion of CH4 was found in the blank experiment in the temperature range of 25–800 °C.
The effluent gas was connected to a gas chromatograph equipped with a HayeSep D (6′ × 1/8″) packed column, a molecular sieve 13 × (6′ × 1/8″) packed column, and a thermal conductivity detector (TCD) for analysis of both reactants and products. The CH4 conversion X% was defined as: . Herein, and are the amounts of pure CH4 at the inlet and outlet of the reactor, respectively. In the CH4 combustion reaction, and can be directly represented by the peak area of CH4 in gas chromatograph before reaction and after reaction, respectively.
In this work all the DFT calculations were carried out with a periodic slab model using the Vienna ab initio simulation program33,39,40,41. The generalized gradient approximation was used with the Perdew-Burke-Ernzerhof42 exchange-correlation functional. Due to the strong correlation effect among the partially filled Co 3d states, we used the Hubbard parameter, U, for the Co 3d electrons to take the on-site Coulomb interaction into account, which is the well-known DFT+U method34. According to previous work29,43, the value of U-J of 2 eV was applied. The projector-augmented wave method44,45 was utilized to describe the electron-ion interactions, and the cut-off energy for the plane-wave basis set was 400 eV. Brillouin zone integration was accomplished using a 2 × 2 × 1 Monkhorst-Pack k-point mesh. All the adsorption geometries were optimized using a force-based conjugate gradient algorithm, while transition states were located with a constrained minimization technique46,47,48.
How to cite this article: Tao, F. et al. Understanding complete oxidation of methane on spinel oxides at a molecular level. Nat. Commun. 6:7798 doi: 10.1038/ncomms8798 (2015).
Zarur, A. J. & Ying, J. Y. Reverse microemulsion synthesis of nanostructured complex oxides for catalytic combustion. Nature 403, 65–67 (2000).
Cargnello, M. et al. Exceptional Activity for Methane Combustion over Modular Pd@CeO2 Subunits on Functionalized Al2O3. Science 337, 713–717 (2012).
Farrauto, R. J. Low-temperature oxidation of methane. Science 337, 659–660 (2012).
Andrushkevich, T. V., Boreskov, G. K., Popovskii, V., Muzikantov, V., Kimhai, O. & Sazonov, V. Kinet. Katal 9, 595 (1968).
Andrushkevich, T. V.,, Boreskov, G. K., Popovskii, V., Pliasova, L., Karakchiev, L. & Ostankovitch, A. Kinet. Katal 9, 1244 (1968).
Papadato, K & Shelstad, K. A. Catalyst screening using a stone DTA apparatus .1. oxidation of toluene over cobalt-metal-oxide catalysts. J. Catal. 28, 116–123 (1973).
Baussart, H., Delobel, R., Lebras, M. & Leroy, J. M. Oxidation of propene on mixed oxides of copper and cobalt. J. Chem. Soc. Farad. T I 75, 1337–1345 (1979).
Prasad, R., Sony & Singh, P. Low temperature complete combustion of a lean mixture of LPG emissions over cobaltite catalysts. Catal. Sci. Technol. 3, 3223–3233 (2013).
Gelin, P. & Primet, M. Complete oxidation of methane at low temperature over noble metal based catalysts: a review. Appl. Catalys. B Environ. 39, 1–37 (2002).
Samsa, M. E. Potential for Compressed Natural Gas Vehicles in Centrally-Fueled Automobile, Truck and Bus Fleet Applications (Gas Research Institute, Chicago, IL, (1991).
Gelin, P., Urfels, L., Primet, M. & Tena, E. Complete oxidation of methane at low temperature over Pt and Pd catalysts for the abatement of lean-burn natural gas fuelled vehicles emissions: influence of water and sulphur containing compounds. Catalys. Today 83, 45–57 (2003).
Honkanen, M. et al. Structural characteristics of natural-gas-vehicle-aged oxidation catalyst. Top. Catal. 56, 576–585 (2013).
Lampert, J. K., Kazi, M. S. & Farrauto, R. J. Palladium catalyst performance for methane emissions abatement from lean burn natural gas vehicles. Appl. Catal. B Environ. 14, 211–223 (1997).
Chin, Y.-H., Buda, C., Neurock, M. & Iglesia, E. Consequences of metal–oxide interconversion for C–H bond activation during CH4 reactions on Pd catalysts. J. Am. Chem. Soc. 135, 15425–15442 (2013).
Zhang, S. R. et al. WGS Catalysis and In Situ Studies of CoO1-x, PtCon/Co3O4, and PtmCom '/CoO1-x Nanorod Catalysts. J. Am. Chem. Soc. 135, 8283–8293 (2013).
Henrich, V. E., & Cox, P. A. The Surface Science of Metal Oxides Cambridge Univ. Press (1994).
Jiang, D. E. & Dai, S. The role of low-coordinate oxygen on Co3O4(110) in catalytic CO oxidation. Phys. Chem. Chem. Phys. 13, 978–984 (2011).
Xie, X. W., Li, Y., Liu, Z. Q., Haruta, M. & Shen, W. J. Low-temperature oxidation of CO catalysed by Co3O4 nanorods. Nature 458, 746–749 (2009).
Wang, L. et al. Catalysis and In-situ Studies of Rh1Con/Co3O4 Nanorods in Reduction of NO with H2 . ACS Catalys. 3, 1011–1019 (2013).
Tao, F. Design of an in-house ambient pressure AP-XPS using a bench-top X-ray source and the surface chemistry of ceria under reaction conditions. Chem. Commun. 48, 3812–3814 (2012).
Klissurski, D. G. & Uzunova, E. L. A comparative-study of the thermal-stability of nickel, copper and zinc spinel cobaltites. Thermochim. Acta 189, 143–149 (1991).
Tao, F. et al. Reaction-Driven Restructuring of Rh-Pd and Pt-Pd Core-Shell Nanoparticles. Science 322, 932–934 (2008).
Zhang, S. R. et al. Restructuring transition metal oxide nanorods for 100% selectivity in reduction of nitric oxide with carbon monoxide. Nano Letters 13, 3310–3314 (2013).
Shan, J. J. et al. Catalytic performance and in situ surface chemistry of pure alpha-MnO2 nanorods in selective reduction of NO and N2O with CO. J. Phys. Chem. 117, 8329–8335 (2013).
Mudiyanselage, K. et al. Importance of the metal-oxide interface in catalysis: in situ studies of the water-gas shift reaction by ambient-pressure X-ray photoelectron spectroscopy. Angew. Chem. Int. Ed. Engl 52, 5101–5105 (2013).
Deng, X. Y. et al. Reactivity differences of nanocrystals and continuous films of alpha-Fe2O3 on Au(111) studied with in situ X-ray photoelectron spectroscopy. J. Phys. Chem. C 114, 22619–22623 (2010).
Deng, X. Y. et al. Surface chemistry of Cu in the presence of CO2 and H2O. Langmuir 24, 9474–9478 (2008).
Wang, W., Su, C., Wu, Y. Z., Ran, R. & Shao, Z. P. Progress in solid oxide fuel cells with nickel-based anodes operating on methane and related fuels. Chem. Rev. 113, 8104–8151 (2013).
Wang, H.-F. et al. Origin of extraordinarily high catalytic activity of Co3O4 and its morphological chemistry for CO oxidation at low temperature. J. Catal. 296, 110–119 (2012).
Wang, Z., Cao, X. M., Zhu, J. & Hu, P. Activity and coke formation of nickel and nickel carbide in dry reforming: a deactivation scheme from density functional theory. J. Catal. 311, 469–480 (2014).
Zhang, C. J. & Hu, P. Methane transformation to carbon and hydrogen on Pd(100): Pathways and energetics from density functional theory calculations. J. Chem. Phys. 116, 322–327 (2002).
Inderwildi, O. R., Jenkins, S. J. & King, D. A. Mechanistic studies of hydrocarbon combustion and synthesis on noble metals. Angew. Chem. Int. Ed. 47, 5253–5255 (2008).
Kresse, G. & Hafner, J. Ab initio molecular dynamics for liquid metals. Phys. Rev. B 47, 558–561 (1993).
Dudarev, S. L., Botton, G. A., Savrasov, S. Y., Humphreys, C. J. & Sutton, A. P. Electron-energy-loss spectra and the structural stability of nickel oxide:An LSDA+U study. Phys. Rev. B 57, 1505–1509 (1998).
Tao, F. et al. Break-up of stepped platinum catalyst surfaces by high CO coverage. Science 327, 850–853 (2010).
Tao, F. & Salmeron, M. In situ studies of chemistry and structure of materials in reactive environments. Science 331, 171–174 (2011).
Zhang, S. et al. In-Situ Studies of Nanocatalysis. Acc. Chem. Res. 46, 1731–1739 (2013).
Zhu, Y. et al. In situ surface chemistries and catalytic performances of ceria doped with palladium, platinum, and rhodium in methane partial oxidation for the production of syngas. ACS Catal. 3, 2627–2639 (2013).
Kresse, G. & Furthmüller, J. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Phys. Rev. B 54, 11169–11186 (1996).
Kresse, G. & Furthmuller, J. Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Comput. Mster. Sci. 6, 15–50 (1996).
Kresse, G. & Hafner, J. Ab-initio molecular-dynamics simulation of the liquid-metal amorphous-semiconductor transition in germanium. Phys. Rev. B 49, 14251–14269 (1994).
Perdew, J. P., Burke, K. & Ernzerhof, M. Generalized gradient approximation made simple. Phys. Rev. Lett. 77, 3865–3868 (1996).
Lv, C.-Q., Liu, C. & Wang, G.-C. A DFT study of methanol oxidation on Co3O4. Catal. Commun. 45, 83–90 (2014).
Kresse, G. & Joubert, D. From ultrasoft pseudopotentials to the projector augmented-wave method. Phys. Rev. B 59, 1758–1775 (1999).
Blöchl, P. E. Projector augmented-wave method. Phys. Rev. B 50, 17953–17979 (1994).
Michaelides, A. et al. Identification of general linear relationships between activation energies and enthalpy changes for dissociation reactions at surfaces. J. Am. Chem. Soc. 125, 3704–3705 (2003).
Liu, Z. P. & Hu, P. General rules for predicting where a catalytic reaction should occur on metal surfaces: A density functional theory study of C-H and C-O bond breaking/making on flat, stepped, and kinked metal surfaces. J. Am. Chem. Soc. 125, 1958–1967 (2003).
Alavi, A., Hu, P. J., Deutsch, T., Silvestrelli, P. L. & Hutter, J. CO oxidation on Pt(111): An ab initio density functional theory study. Phys. Rev. Lett. 80, 3650–3653 (1998).
F.T. acknowledges the funding support from the Chemical Sciences, Geosciences and Biosciences Division, Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy under Grant No. DE-FG02-12ER16353.
The authors declare no competing financial interests.
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Tao, F., Shan, Jj., Nguyen, L. et al. Understanding complete oxidation of methane on spinel oxides at a molecular level. Nat Commun 6, 7798 (2015). https://doi.org/10.1038/ncomms8798
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