Controlling the structure of catalysts at the atomic level provides an opportunity to establish detailed understanding of the catalytic form-to-function and realize new, non-equilibrium catalytic structures. Here, advanced thin-film deposition is used to control the atomic structure of La2/3Sr1/3MnO3, a well-known catalyst for the oxygen reduction reaction. The surface and sub-surface is customized, whereas the overall composition and d-electron configuration of the oxide is kept constant. Although the addition of SrMnO3 benefits the oxygen reduction reaction via electronic structure and conductivity improvements, SrMnO3 can react with ambient air to reduce the surface site availability. Placing SrMnO3 in the sub-surface underneath a LaMnO3 overlayer allows the catalyst to maintain the surface site availability while benefiting from improved electronic effects. The results show the promise of advanced thin-film deposition for realizing atomically precise catalysts, in which the surface and sub-surface structure and stoichiometry are tailored for functionality, over controlling only bulk compositions.
Understanding the structure–activity relationship of a catalyst at the atomic level has been a long-standing challenge in the pursuit of a designer catalyst1,2,3,4,5. Traditionally, researchers identify this relationship by varying the bulk structure and/or composition and examining the impact on the catalytic performance. Although these efforts have resulted in design principles and discoveries of new catalysts, options beyond bulk variable control have not been fully explored. Advances in non-platinum catalysts such as carbon-based and metal-oxide catalysts for alkaline conditions further accentuate the need for full exploration of catalyst design beyond bulk variable control6,7. An emerging concept is to independently tune the structure and composition in the surface and sub-surface layers, the layers most sensitive to surface reactions. Control of these parameters provide the allure of optimizing electronic structure and surface chemistry in separate but closely coupled atomic layers8,9. Independently controlling the surface and sub-surface structure and composition, however, requires the ability to prepare materials with atomic precisions in a non-equilibrium manner. This often presents a practical obstacle for materials scientists. The purpose of this article is to present a route to realize this concept via advanced thin-film deposition.
Studies of well-defined single crystals have shown that the sub-surface atoms play an important role on the catalytic performance just as the surface atoms10,11,12,13,14,15. Driven by these findings, many researchers have synthesized catalysts with core-shell structures to manipulate the performance of the catalyst by using heat treatment to induce surface segregation or via post-synthetic deposition16,17,18,19. These syntheses, however, do not afford the ability to control the surface and sub-surface structure and composition in a systematic fashion. As a result, it has not been straightforward to obtain the structure–activity relations from these experiments. The difficulty in controlling the surface and sub-surface structure and composition is particularly challenging for oxide catalysts used in alkaline fuel cells and metal-air batteries, where complex quaternary phase diagrams and high-temperature treatment used for preparations often push the catalyst to favor the equilibrium structure20,21,22,23,24,25,26.
Here, this difficulty is tackled through advanced thin-film deposition. Thin films of La2/3Sr1/3MnO3 are grown layer-by-layer by molecular beam epitaxy (MBE). The surface and sub-surface compositions of the films were varied by tuning the deposition sequence while maintaining the overall stoichiometry and identical electronic structure. Comparison of the catalytic activity of the films for oxygen reduction reaction (ORR) show that the placement of the SrMnO3 layer in the sub-surface shows greater activity than when SrMnO3 is placed on the surface. Ambient pressure X-ray photoelectron spectroscopy (APXPS) reveals that the SrMnO3 layer improves the electronic structure and conductivity for ORR, but simultaneously reacts with ambient air to reduce the number of active sites. Placing SrMnO3 in the sub-surface is the optimal choice for the film to maximally benefit from the former effect, whereas minimizing the latter.
Film growth and structural characterization
In all, 20-nm thick La2/3Sr1/3MnO3 heterostructures were grown by MBE on TiO2-terminated (001) SrTiO3 single-crystal substrates27. (001) was chosen as the low-energy termination of the perovskite structure which allows for a layer-by-layer growth. The structural integrity of the heterostructures were characterized using four-circle X-ray diffraction (XRD), angle-resolved photoemission spectroscopy (ARPES), and transport measurements28,29. These results also show that thin films studied in this article, thin films of low repeat units (n = 1 and 2), the LaMnO3 and SrMnO3 layers are commensurate to the substrate and the effects of interlayer strain are very small. For comparison, we study LaMnO3 (LLL) and La2/3Sr1/3MnO3 (where La and Sr form a solid solution) films of the same thickness. For (LaMnO3)2/(SrMnO3), we permute the ordering between LaMnO3 and SrMnO3 to control the SrMnO3 placement at either the surface, sub-surface, and sub-sub-surface. Films are referred to be based on their repeat units: SrMnO3-LaMnO3-LaMnO3 as “SLL”, LaMnO3-SrMnO3-LaMnO3 as “LSL”, and LaMnO3-LaMnO3-SrMnO3 as “LLS” (Fig. 1). In this nomenclature, the first letter of the name represents the layer that is closest to the surface. We follow the same naming convention for (LaMnO3)4/(SrMnO3)2, where we prepare LLSSLL and SSLLLL as our model (LaMnO3)4/(SrMnO3)2 heterostructures (Supplementary Figure 1). X-ray analysis shows reflections from both the perovskite structure and the superlattice (Fig. 2a and Supplementary Figure 2).
To verify the SrMnO3 placement, we measure the intensity ratios between the raw La 4d and Sr 3d peaks using APXPS. For excitation energies that correspond to probing depths of around one functional unit (~1.1 nm) from the surface (photon energies of 340 eV for La 4d and 385 eV for Sr 3d), the APXPS results show that LLS has the highest La/Sr intensity ratio near the surface, followed by LSL, and then SLL (Fig. 2b). These compositional ratios agree with our intended SrMnO3 placement and are unchanged under different pO2 (Fig. 2b). The consistent compositional ratios support our naming nomenclature and our assignment of any observed difference in the ORR activity to the SrMnO3 placement within the heterostructures.
ORR activity comparison
The surface and sub-surface placement plays an important role on the ORR. Figure 3a shows the ORR activity on (LaMnO3)2/(SrMnO3) heterostructures in a Tafel plot. All (LaMnO3)2/(SrMnO3) heterostructures share the same Tafel slope, suggesting a similar reaction pathway (for the studied composition, the overall reaction is O2 + 2H2O + 4e– → 4OH–24). As our analysis focuses on the current range that is much smaller than the mass transport limit30, we did not apply any diffusion correction. For a visual comparison, Fig. 3b shows the ORR current at 0.8 V vs. reversible hydrogen electrode (RHE). LSL, where the Sr layer resides in the sub-surface layer, is the most active, followed by SLL, LLS, and then LLL. The low activity of LLS suggests that Sr most efficiently benefits ORR when it is placed within two-unit cells from the surface Mn (<1 nm). As Sr benefits ORR by affecting the d-electron configuration of Mn in the eg symmetry20, the low activity of LLS indicates that electronic effect of Sr is localized to approximately two-unit cells. This hypothesis is consistent with the observation that the ORR kinetics on (LaMnO3)2/(SrMnO3) is more active than (LaMnO3)4/(SrMnO3)2; both LLSSLL and SSLLLL (Supplementary Figures 3, 4) reveal that larger superlattice spacing impedes Sr from benefiting the topmost Mn layer for ORR. This interpretation of our results agrees with previous ARPES experiments and first-principle calculations. ARPES showed reduced electronic hopping integrals when the spacing between the LaMnO3 and SrMnO3 layers increases28. First-principle calculations showed that the charge transfer effects of the (LaMnO3)2/(SrMnO3) interfaces are confined to ~2-unit cells31,32. Comparing the electrochemical behavior of (LaMnO3)2n/(SrMnO3)n (n = 1, 2) to that of a random alloy (‘Alloy’) further reveals the effects of sub-surface engineering (Supplementary Figure 5). The Alloy film, which should structurally represent a random mixture of the three (LaMnO3)2/(SrMnO3) films, performs close to the average of the three films, markedly poorer than LSL (Supplementary Figure 5). Both our results and those in the literature from the electronic structure community confirm a long-held intuition: sub-surface chemistry manipulation is the most direct way to influence the activity of the topmost catalytic layer, and that the effect gradually decreases as the manipulation occurs on a layer further away from the surface.
Having concluded the positive role of the near-surface La-Sr interface, we can now discuss why ORR is more active when Sr is placed in the sub-surface (LSL) compared with when Sr is placed on the surface (SLL). Stoerzinger et al. have shown that the charge transfer capability in La1-xSrxMnO3 (measured using the [Fe(CN)6]3−/4− outer sphere redox reaction) depends on x, the Sr content. Their results suggested that in addition to tuning the eg occupation, the Sr addition also benefits the ORR activity of LaMnO3 by providing carriers to increase conductivity30. Interestingly, we observe no difference in the charge transfer capabilities between LLS, LSL, and SLL, for the same [Fe(CN)6]3−/4− outer sphere redox reaction (Supplementary Figure 6). Therefore, the availability of transferrable electrons does not explain the ORR difference between SLL, LSL, and LLS (Fig. 2). The observation that (LaMnO3)2/(SrMnO3) is not limited by the availability of transferrable electrons is consistent with the transport measurements, which showed that (LaMnO3)2/(SrMnO3) is metallic29,33,34.
With conductivity ruled out, we study the surface chemistry and electronic structure using APXPS. Supplementary Figure 7 shows the valence band spectra at low-energy (340 eV, inelastic mean free path, IMFP, ~0.6 nm) and high-energy (780 eV, IMFP, ~1.3 nm) excitations in both vacuum (pO2 < 10−9 Torr) and near-ambient pressure (pO2 ~ 10−1 Torr). The valence spectra of La1-xSrxMnO3 is principally assigned to a combination of the O 2p (6 eV) and Mn 3d states (2 eV)35,36,37,38. As we move from deeper probing depth (~1.3 nm) to shallower probing depth (~0.6 nm), the valence spectra undergo a spectral weight transfer from the high-energy edge to about 2 eV from the Fermi level. This change is attributed to the surface localization, which reduces the bandwidth and produces a localized, narrow Mn 3d state at the surface. These experiments have two implications. First, the use of a molecular orbital model is a reasonable approximation for the oxide surfaces given the localized nature of the Mn d-state. Second, even with synchrotron APXPS, the difference in the valence band spectra between the superlattices are not resolvable. We have therefore focused our analysis on the core spectra, which have superior signal-to-noise ratios.
The core spectra provide insight into the surface chemistry difference between LSL and SLL. Background-subtracted spectra show that La 4d peaks are insensitive of the SrMnO3 placement and the pO2 level (Supplementary Figure 8). This observation indicates that La is mostly a spectator and does not interact with atmospheric oxygen. We similarly observe that Sr 3d peaks in LSL and LLS do not change with pO2, which is consistent with the idea that the sub-surface and sub-sub-surface Sr cannot “see” atmospheric oxygen (Supplementary Figure 9). However, for SLL, APXPS reveals that Sr can react with oxygen to form Sr-oxide-like species (Fig. 4, Supplementary Figure 9). This surface Sr component (~135 eV) grows systematically with pO2 (Fig. 5, see Supplementary Figure 9 and Supplementary Table 1 for spectra analysis). Surface segregation of Sr-oxide like species have been observed for La1-xSrxMnO3 powders, pellets, and films39,40,41. We similarly believe that the top SrO layer within the superlattice could segregate past the top MnO2 layer to form Sr-oxide species on the surface of SLL. These observations suggest that the formation of the surface Sr-oxide could block the oxygen access to the surface Mn once the catalyst is exposed to atmospheric oxygen during the ORR. In this picture, LSL is more active than SLL because SrMnO3 resides in the sub-surface layer. Even though their surfaces nominally share the same local electronic structure, LSL surface is more accessible due to the absence of blocking Sr oxides.
Surface site availability for oxygen adsorption plays a critical role in ORR on Pt. Stamenkovic et al. have suggested that the surface site availability enhances the ORR activity on Pt3Ni(111)10. We believe that a similar phenomenon occurs for the LSL heterostructure. The presence of Sr in LaMnO3 (i.e., La2/3Sr1/3MnO3), although beneficial by modifying the eg occupation of the Mn to increase the ORR activity, can simultaneously reduce the surface site availability by forming a surface Sr-oxide group that restricts the oxygen access to the active Mn sites. Strmcnik et al. have previously suggested that the surface oxide species could reduce the surface site availability by interacting with the ions in the electrochemical double layer42. This scenario is also possible in our superlattices.
Our result shows the double-edged effect of Sr in La2/3Sr1/3MnO3, where Sr can promote ORR by modifying the Mn electronic structure, but suppress the surface site availability when placed too close to the surface. The double-edged effect may explain why increasing the Mn valence state by oxygen overstoichiometry (e.g., LaMnO3+ δ) results in a more active catalyst than by aliovalent substitutions (e.g., La1-xCaxMnO3), despite both leading to Mn catalysts with nearly the same Mn oxidation state and crystal structure20. We emphasize, however, that this is unlikely the only effect. As recently highlighted, Mn perovskite oxides are more active when synthesized using a co-precipitation method20,43,44. Defects and surface segregation likely play a critical role also. Finally, we note that we were unable to resolve major differences between the superlattices in either the valence band spectra, O 1s (K-edge), or Mn 2p (L-edge) X-ray absorption (Supplementary Figures 10, 11), which likely points to the need for higher resolution, higher efficiency X-ray techniques, especially new detector technologies that can resolve local electronic structure in the near-surface layer. Previous X-ray studies on La1-xSrxMnO3 have shown only subtle changes in valence band for 0.3 ≤ x ≤ 0.6 despite observable differences in electronic properties35,45. Developing finer resolution spectroscopy methods is an essential future step to reveal the nature of surface bonding in transition-metal oxides designed with customized surface and sub-surface.
Our investigation of the surface and sub-surface customizations of La2/3Sr1/3MnO3 reveals that ORR is most active when SrMnO3 resides in the sub-surface vs. when it resides in the surface, the sub-sub-surface, or randomly distributed. APXPS reveals that this observation stems from the double-edged effect of Sr, which benefits ORR by modifying the electronic structure of the Mn sites, but can also form non-catalytic Sr oxides that reduce the surface site availability. Analysis of the valence band and elemental peak spectra in the presence of oxygen reveals that Sr modifies the electronic structure but also reacts to form a detrimental oxide species when present in the surface layer. Our finding demonstrates the Goldilocks effect, where moving the Sr closer to the surface allows the surface Mn atoms to more efficiently catalyze ORR, but Sr at the surface poisons the catalyst and reduces functionality. As a result, the catalyst is most active when the surface and sub-surface layer are LaMnO3 and SrMnO3, respectively. Most importantly, our work points to an opportunity to design an ORR catalyst by customizing surface and sub-surface stoichiometry, orientation, and structure. The ability to control both parameters independently and rationally with atomic-layer precision can lead to the discovery of new catalysts with functionalities superior to those accessed through traditional bulk-composition control.
Epitaxial (LaMnO3)2n/(SrMnO3)n (n = 1, 2) superlattices were deposited on (001)-SrTiO3 single crystals using MBE. LaMnO3 (LLL), La2/3Sr1/3MnO3 and five superlattices (LLS, LSL, SLL, LLSSLL, and SSLLLL) were prepared using a layer-by-layer deposition. In all synthesized heterostructures, the first letter represents the surface layer. All films were terminated with the Mn layer and XRD confirms the pseudo-cubic perovskite structure.
To establish the connection between the surface and sub-surface customizations and electronic structure, we use APXPS46 to monitor the surface chemistry of the heterostructures. APXPS measurements were collected at Beamline 9.3.2 at the Advanced Light Source (ALS) of the Lawrence Berkeley National Laboratory (LBNL). After loading, all samples were heated to and held at 200 °C at 1 mTorr pO2 for 30 min to remove surface adsorbed organics, which were monitored via the C1s spectra. We tune to the excitation energy such that the kinetic energy of the escaping electron is uniformly 250 eV for all elemental peaks. This kinetic energy corresponds to a probing depth of around one functional unit (~1.1 nm). The following elemental peaks were measured (at the specified excitation energies): O 1s (780 eV), Sr 3d (385 eV), and La 4d (340 eV). During the core peak measurements, we simultaneously collect the valence spectra. La 4d XPS peaks were calibrated to the leading edge of the La 4d peaks to be at 100 eV as La peaks are qualitatively unaffected by changes in pO2 (Fig. S1). Other peaks were calibrated with respect to the La 4d peaks of the same sample and pressure by aligning the O 2p edge of the valence band spectra (7–8 eV) to the calibrated valence band spectra of the La 4d peaks with an error of ± 0.1 eV. We use a Shirley background correction. We also collected Mn L-edge and O K-edge X-ray absorption spectra in a partial-electron-yield mode in the same conditions as APXPS. All spectra were normalized to the background absorption below and above the absorption edge.
Electrochemical measurements were conducted in a standard three-electrode cell (Pine) using a potentiostat (Bio-Logic). The reference electrode was a Ag/AgCl redox couple in a saturated KCl solution, calibrated to the H2/H+ redox. The ohmic resistance correction used the high-frequency real-axis intercept of the impedance measurement. Front contacts were made using gallium-indium eutectic (Sigma-Aldrich, 99.99%) and silver paint (Ted Pella, Leitsilber 200) for electrical contact. The contact and the sides and back of the substrate were all covered with epoxy (Omegabond 101) to ensure electrochemical insulation of these regions30. All samples were front contacted to avoid passing the current through the film-substrate interface. The ORR measurements were conducted in O2-saturated (Airgas, ultrahigh-grade purity) 0.1 M KOH, prepared from Milli-Q water (18.2 Ω∙cm, Millipore) with KOH pellets (Sigma-Aldrich, 99.99%) at a rate of 10 mV/s. The ORR curves were obtained by subtracting the ORR current measured in O2 vs. background current measured in Ar (Airgas, ultrahigh-grade purity) in 0.1 M KOH. The ORR activity is from the third cycle, where the subsequent scan did not vary by >5% of the previous scan. The error bars represent the standard deviations for at least three independent measurements. The [Fe(CN)6]3−/4− measurements were conducted in Ar-saturated 0.1 M KOH solution with 5 mM K4Fe(CN)6∙3H2O (Alfa Aesar, 98.5–102.0%) and K3Fe(CN)6 (Alfa Aesar, 99%) at a rate of 10 mV/s.
The data that support the findings of this study are available from the authors on reasonable request.
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We acknowledge Amit Bhatia, Runbang Tang, Chengyu Liu, and Kevin E. Fritz for their help with the X-ray measurements, and Elizabeth A. Nowadnick (‘Beth’), Jason K. Kawasaki, and Julia A. Mundy for insightful discussions. This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Award Number DE-SC-0018029. This work made use of the Cornell Center for Materials Research (CCMR) Shared Facilities, which are supported through the NSF MRSEC program (DMR-1120296). The Advanced Light Source is supported by the Director, Office of Basic Energy Sciences, of the U.S. Department of Energy under contract no. DE-AC02-05CH11231. C.A. and D.G.S. acknowledge funding from the National Science Foundation under grant no. DMR-1610781. E.J.M. and S.J.M. acknowledge funding from the Army Research Office (W911NF-15-1-0133). Substrate preparation was performed in part at the Cornell NanoScale Facility, a member of the National Nanotechnology Coordinated Infrastructure (NNCI), which is supported by the National Science Foundation (grant ECCS-15420819).
The authors declare no competing interests.
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Eom, C.J., Kuo, DY., Adamo, C. et al. Tailoring manganese oxide with atomic precision to increase surface site availability for oxygen reduction catalysis. Nat Commun 9, 4034 (2018). https://doi.org/10.1038/s41467-018-06503-8
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