Significance
Metal-oxide catalysts that do not rely on the critical metals corrode immediately in nonbasic solutions. The development of self-healing offers a design principle to avert corrosion for typical metal oxides in neutral and near-neutral solutions. However, the stabilization of metal-oxide oxygen evolution catalysts (OECs) in acid remains to be a challenge that requires new design principles and strategies. We show here that high activity from OECs may be achieved in acid by embedding catalytic metal-oxide active sites within an acid-stable oxide framework. Specifically, we show that oxidic Ni OECs may be stabilized for extended periods of OER by embedding Ni in the acid-stable oxide framework of PbO2 polymorphs.
Keywords: water-splitting catalysis, renewable energy, solar to fuels, electrocatalysis, acid-stable templating
Abstract
Earth-abundant oxygen evolution catalysts (OECs) with extended stability in acid can be constructed by embedding active sites within an acid-stable metal-oxide framework. Here, we report stable NiPbOx films that are able to perform oxygen evolution reaction (OER) catalysis for extended periods of operation (>20 h) in acidic solutions of pH 2.5; conversely, native NiOx catalyst films dissolve immediately. In situ X-ray absorption spectroscopy and ex situ X-ray photoelectron spectroscopy reveal that PbO2 is unperturbed after addition of Ni and/or Fe into the lattice, which serves as an acid-stable, conductive framework for embedded OER active centers. The ability to perform OER in acid allows the mechanism of Fe doping on Ni catalysts to be further probed. Catalyst activity with Fe doping of oxidic Ni OEC under acid conditions, as compared to neutral or basic conditions, supports the contention that role of Fe3+ in enhancing catalytic activity in Ni oxide catalysts arises from its Lewis acid properties.
Widespread implementation of solar energy requires the utilization of efficient energy storage systems that manage the diurnal nature of solar sources (1–4). Hydrogen storage coupled with fuel cells (5), and electrochemical water electrolysis to generate oxygen and hydrogen coupled to CO2 fixation (6, 7) offer portable solutions to energy storage. Of the two water-electrolysis half reactions, the oxygen evolution reaction (OER) is more kinetically demanding because it requires the transfer of four protons coupled with four electrons from two water molecules to produce a single oxygen molecule (8–10).
A variety of earth-abundant metal oxides have been developed to operate OER in both neutral and basic pH regimes (11–19), but they are unstable in acid, undergoing rapid dissolution into soluble metal ions. The development of oxygen-evolving catalysts (OECs) that operate in acid is desirable in the application of electrolyzers (20, 21) and selected photoelectrochemical devices (22, 23), due to the creation of locally acidic environments by Nafion membranes and requisite acidic pH for silicon-based photovoltaic material stability, respectively. IrO2 and RuO2 have high activity for OER and long-term stability in acid but they are composed of critical metals thus prohibiting their widespread adoption (24, 25). Efforts have been made to enhance MnOx films, which form stable oxides in low-pH regimes (26), for OER through potential cycling deposition (27, 28). These films, however, do not operate at high current densities for extended periods of time owing to phase and compositional transitions of the manganese oxide lattice. To develop a robust and active catalyst for OER in acid using earth-abundant metals, we have pursued a mixed-metal-oxide design strategy with each metal oxide serving an independent role to optimize stability and activity. We have previously demonstrated this design concept with the development of CoFePbOx which satisfies the criteria of an idealized OEC in acid (29) by utilizing the acid stability and conductivity of PbOx. These films showed extended stability in acid at appreciable OER currents and high activity.
We sought to stabilize NiBi and (Ni:Fe)Bi OECs in acid owing to their exceptional OER activities, especially for the latter (30, 31). We show herein that NiFePbOx and NiPbOx films are stable in acid through extended OER electrolysis (>20 h) as compared to NiBi, NiOx, and NiFeOx films, all of which dissolve within minutes under the same conditions. X-ray spectroscopy reveals that the PbOx-framework is stable under OER conditions in acid. Because the mixed-oxide strategy stabilizes the catalyst, we are able to examine OER in acid, especially the issue of Fe as a promoter of catalysis. Many interesting explanations for the enhanced OER activity of oxidic Ni OER catalysts alloyed with Fe have been posited including active-site Fe species (17, 32–37), near-neighbor Fe effects on OER at Ni resulting from strain on the oxide lattice (38, 39) or as a relay of active oxygen intermediates to Ni (40–42), and Fe-inducing partial-charge-transfer activation of Ni for OER generation (17). We have suggested (43), based on X-ray absorption spectroscopy of (Ni:Fe)Bi, that a role of Fe is to act as a Lewis acid, serving to increase the acidity of OHx (aqua/hydroxo) moieties that are coordinated to nickel, thereby lowering the reduction potential for the Ni3+/4+ couple, leading to a greater population of Ni4+ in the Fe-doped catalysts. This in turn gives rise to increased oxyl character arising from a Ni(IV)O ↔ Ni(III)–O• resonance, which leads to facilitated O–O bond formation. Whereas the Lewis acidity [pKa = 2.2 (44)] of Fe3+ may be manifested in near-neutral and basic solutions, in more acidic solutions the effect should be mitigated. We indeed show that Fe doping in NiPbOx shows no enhancement in OER at solution pH values commensurate with the pKa of Fe3+. Taken together, our findings establish general guidelines for how catalysts may be designed to optimize both OEC activity and stability in acid.
Results
Performance of NiPbOx and NiFePbOx Films in Acid.
NiFePbOx and NiPbOx films were electrodeposited at a constant anodic potential of 1.3 V vs. NHE from aqueous solutions containing the appropriate metal salts and methylphosphonate (MePi) buffer at pH 8, similar to previously published methods (SI Appendix, Fig. S1) (29); PbOx and FePbOx films were similarly prepared. The deposition times for all films were chosen so as to yield ∼250 nmol in total metal loading as confirmed by inductively coupled plasma mass spectrometry (ICP-MS) (SI Appendix, Table S1). The as-deposited NiPbOx films contain equal parts Ni (50.3 ± 0.3 mol %) and Pb (49.7 ± 1.2 mol %). Likewise, the as-deposited NiFePbOx films also contain approximately equal parts Ni (30.1 ± 0.6 mol %), Fe (30.9 ± 1.2 mol %), and Pb (39.0 ± 0.8 mol %).
The morphology of each film was examined by scanning electron microscopy (SEM) (SI Appendix, Fig. S2). PbOx films appear to be filament-like whereas NiPbOx appear to be more nanoparticlelike in morphology; comparing NiPbOx and NiFePbOx, the addition of Fe appears to change the morphology by decreasing the size of the nanoparticle structures. Average particle diameters of ∼150 and ∼70 nm are observed for NiPbOx and NiFePbOx, respectively. Energy-dispersive X-ray spectroscopy (EDS) mapping shows a uniform distribution of elements throughout the surface of all films (SI Appendix, Fig. S3). The amorphous nature of PbOx-templated films precluded the use of X-ray diffraction as a characterization tool.
The stabilities of PbOx-based films (mixed-metal-oxide films employing a lead-oxide lattice framework) were evaluated with chronopotentiometry in 0.1 M KPi + 1.75 M KNO3 solutions at pH 2.5 (Fig. 1). Electrodeposited films were immersed in stirred solutions and held at a constant current density of 1 mA cm–2 where, after a brief capacitance period, only OER was sustained. The applied potentials required to maintain 1 mA cm–2 of OER (V1mA) for NiFePbOx and NiPbOx films initially stabilize at a value well below that of blank fluorinated tin oxide (FTO) (SI Appendix, Fig. S4A). This potential is maintained for >20 h before rapidly rising to the value for OER on FTO. Both NiFePbOx and NiPbOx films have superior acid stability over NiOx, NiFeOx, and NiBi films, which immediately dissolve in acidic conditions (Fig. 1 and SI Appendix, Fig. S4B), whereas PbOx and FePbOx perform OER at a V1mA similar to blank FTO. Addition of Fe into NiPbOx increases the stability of the film in acid (Fig. 1 and SI Appendix, Fig. S4B) but does not influence V1mA (SI Appendix, Fig. S4A). To confirm that all electrons consumed are used for OER, the faradaic efficiency of NiFePbOx was measured under operation at 1 mA cm–2 by chronopotentiometry in 0.1 M KPi + 1 M KNO3 pH 2.5. The evolved oxygen was directly measured by gas chromatography from a gas-tight electrochemical cell and the O2 concentration was sampled every 20 min after an initial 30 min of purging the gas headspace with Ar. The faradaic efficiency of NiFePbOx for oxygen generation was 103 ± 3% (SI Appendix, Fig. S5).
To determine the activity of NiFePbOx and NiPbOx films for OER, Tafel plots were measured in 0.1 M KPi + 1 M KNO3 pH 2.5 buffer. Both NiFePbOx and NiPbOx films display a similar Tafel slope of ∼90 mV/dec (Fig. 2), which is similar to that of NiFePbOx at pH 7 (SI Appendix, Fig. S6) and NiOx in near-neutral and basic conditions (15–17). Increasing the amount of Fe in the film relative to Ni results in an increase in the Tafel slope of NiFePbOx films (SI Appendix, Fig. S7A) with a concomitant increase in V1mA (SI Appendix, Fig. S7B). Additionally, cyclic voltammograms performed with NiPbOx and NiFePbOx films in 0.1 M KPi + 1 M KNO3 pH 2.5 buffer show that the OER activity of the two films is very similar (SI Appendix, Fig. S13). A slight reduction in the size of the precatalytic redox feature for the NiFePbOx film is observed, likely due to the reduced Ni content of the Fe-containing film. The OER enhancement of Fe on Ni is thus not observed in NiFePbOx under acidic conditions.
X-Ray Absorption Spectroscopy of PbOx Based Films.
X-ray absorption spectroscopy (XAS) was utilized to assess the in situ geometric and electronic structure of NiFePbOx and to assess changes to the PbOx lattice that may be induced by the addition of Ni and Fe centers. The Pb L3 edge of in situ NiFePbOx (operated at 1.7 V in 0.1 M KPi and 1 M KNO3 pH 2.5 buffer) is given in Fig. 3A, along with data for Pb(II)O, Pb(II,IV)3O4, and Pb(IV)O2. Depending on the oxidation state, the Pb L3 edge comprises three or four transitions from the Pb 2p3/2 state (45, 46). Band (I) is present in Pb(IV)-containing compounds and arises from a Pb 2p3/2 → 6s1/2 transition [oxidation of Pb(II) to Pb(IV) opens up this dipole-allowed transition that is not present in Pb(II) compounds due to the filled 6s2 electronic configuration]. Thus, the in situ L3-edge XAS data support a Pb(IV) oxidation state in NiFePbOx under OER conditions, as expected based on the Pourbaix diagram of lead. There are some differences between the Pb(IV)O2 standard and in situ NiFePbOx in terms of intensity distributions over the higher-energy transitions making up the L3 edge. As these transitions involve final states with mixed Pb 6p1/2/d3/2 and Pb 6d nonbonding and antibonding character, this energy region may reflect partial covalent interaction between unoccupied Pb 6d and occupied Ni and/or Fe orbitals. All PbOx films operating under anodic potentials (1.7 V) in acid exhibit similar Pb L3-edge XAS spectra (Fig. 3B). Moreover, the presence of Ni and/or Fe in PbOx does not appear to significantly influence the L3-edge energies or overall spectral shape.
The PbOx framework was also examined by X-ray photoelectron spectroscopy (XPS). Addition of any other metal into the PbOx framework results in a shift of the Pb 4f peaks toward higher binding energies (Fig. 4A). The Pb 4f binding energies for FePbOx and NiFePbOx appear roughly aligned, and NiPbOx has the highest Pb 4f binding energies. The O 1s XPS spectra of PbOx show peaks at ∼529 eV, a major peak at ∼530 eV, and a small shoulder at ∼532 eV (Fig. 4B). The peak at 529 eV disappears when any metal is added into the PbOx framework. FePbOx and NiFePbOx films all have similar O 1s spectra consisting of one dominant peak at 530.7 eV and a small shoulder at 532 eV. For PbOx and NiPbOx there is a dominant peak at 530 eV and a prominent shoulder at 532 eV; the latter is diminished with the addition of Fe into the framework. The Pb 4f and O 1s XPS spectra of PbOx films do not show any significant changes in binding energy or shape for samples that were held at 1.45 V versus those held at 2.00 V. This indicates that the observed shifts in Pb 4f binding energy are not the result of the various potentials (1.45–2.0 V) applied to PbOx-based films. Consistent with XAS results, the addition of Fe (∼11 mol % Fe) into the NiPbOx film yielded no changes in the XPS spectrum in the Ni 2p region (SI Appendix, Fig. S8).
To understand the electronic changes occurring at the metal and oxygen centers throughout operation of OER in acid, ex situ XAS and XPS spectra of NiFePbOx were examined. Under OER conditions in acid, the influence of Fe on Ni centers within the PbOx framework is minimal. The Ni K edge in the XAS spectrum of NiFePbOx is slightly red-shifted compared to that of NiPbOx (SI Appendix, Fig. S9; 12.9 ± 5.2% Fe), similar to what has been observed for NiFeOx operating OER in base (47) and NiFeBi in near-neutral buffers (43). For the case of the PbOx lattice, the XPS spectra of Pb 4f, Ni 2p, and O 1s in NiFePbOx were tracked over several hours until film dissolution in 0.1 M KPi + 1 M KNO3 pH 2.5 (SI Appendix, Fig. S10). The Pb 4f peaks are shifted toward higher energies in NiFePbOx films that operate 1 mA cm–2 of OER for 40 h (past film stability) versus those films operating 1 mA cm–2 of OER for 10 min. The O 1s peaks are also shifted toward higher energies, and intensity of the peak at 532 eV increases after 40 h of OER. The amount of Ni left on the surface of the FTO substrate is below detection level for XPS analysis. This suggests that the shift toward higher binding energies is likely due to the oxidation of metal centers at the significantly higher potential (2.7 V) required to achieve 1 mA cm–2 of OER after film dissolution.
Catalyst Composition throughout OER.
We compared the elemental composition of as-deposited PbOx-based films with films that had deactivated following 40 h of OER at 1 mA cm–2 in 0.1 M KPi + 1 M KNO3 pH 2.5 (SI Appendix, Fig. S11 and Table S1). After performing OER for 40 h, films exhibit a notable loss of Ni and Fe, which is expected given their propensity to dissolve in acid as predicted by the Pourbaix diagram. NiPbOx films show an ∼99% loss of Ni relative to as-deposited films, while NiFePbOx films show ∼96 and ∼88% loss of Ni and Fe, respectively, relative to as-deposited films. Both NiPbOx and NiFePbOx films have similar Pb loading (relative to as-deposited films) after 40 h. To observe changes in film morphology and structure during operation, the elemental maps of the Pb M edge on NiFePbOx film surfaces were tracked at different time points during operation of 1 mA cm–2 of OER in 0.1 M KPi + 1 M KNO3 pH 2.5 (Fig. 5 and SI Appendix, Fig. S12). Mapping of the Pb M edge on these film surfaces reveals a systematic etching of the PbOx lattice; the film starts out with a uniform Pb distribution that breaks apart to form islands that become more separated over time.
Discussion
NiFePbOx and NiPbOx OER Activity in Acid.
NiPbOx and NiFePbOx films have a homogeneous dispersion of metal centers (SI Appendix, Fig. S3) and exhibit extended stability in acid while maintaining 1 mA cm–2 of OER (Fig. 1). The addition of Fe into the NiFePbOx framework extends the film stability by ∼8 h in contrast to NiBi, NiOx, and NiFeOx films, all of which dissolve within the first few minutes of OER operation in acid (SI Appendix, Fig. S3B).
While Fe has been shown to improve the OER activity of NiOx films in base (17, 48), it does not appear to play a significant role in the enhancement of OER in acid. Both NiFePbOx and NiPbOx yield a Tafel slope of ∼90 mV/dec in acidic conditions (Fig. 3A and SI Appendix, Fig. S7A), which matches that exhibited by pure NiOx in near-neutral and basic conditions (17, 48). Additionally, both the exchange current density and the V1mA scale with Ni rather than Fe content (SI Appendix, Fig. S7). The absence of Fe enhancement in acid is inconsistent with the proposed role of Fe as the active site for OER in Ni:Fe oxide films (17, 32–36). ICP-MS analysis of NiFePbOx films shows an ∼30 mol % Ni and ∼30 mol % Fe composition. Elemental mapping by SEM/EDS illustrates a uniform distribution of metals on the film surface (SI Appendix, Fig. S3D). Furthermore, when operated in near-neutral (pH 9.2) solutions, NiFePbOx yields a lower Tafel slope of 48 mV/dec (SI Appendix, Fig. S6B). These three observations suggest that Fe centers are likely proximate to Ni in the PbOx matrix and are thus not prohibitively diluted to prevent Fe enhancement of OER as suggested by active-site models. It is noteworthy that the observed 48-mV/dec Tafel slope for NiFePbOx at pH 9.2 is similar to that of NiBi (16), suggesting that the nature of the OER active sites in these films at near-neutral pH are similar to NiBi. Rather, the absence of an Fe effect on OER is consistent with the proposal of Fe’s role as a superior Lewis acid promoter of OER (43). The percent of Fe3+ doping promotes the formation of formal Ni4+, which in turn directly correlates with an enhanced activity of the catalyst in promoting OER. This observation has been ascribed to the presence of Lewis acidic Fe3+ serving to increase the acidity of OHx (aqua/hydroxo) moieties that are coordinated to nickel, thereby lowering the reduction potential for the Ni3+/4+ couple and engendering a greater population of Ni4+ in the Fe-doped catalysts. Computation and experiment show Fe3+ to be the most acidic transition metal ion with a pKa = 2.2 for the deprotonation of coordinated water (44). Thus, the Lewis acidity of Fe3+ will be manifested in the enhancement for OER performed in near-neutral conditions but not under the conditions reported here (pH = 2.5) as the pKa of Fe3+ is commensurate with the solution acidity.
Structural Analysis of PbOx Films.
The similarity of Pb L3-edge XAS data shown in Fig. 3 suggests that the Pb(IV)O2 host structure is not greatly perturbed by Ni and Fe doping. Such behavior has been observed previously for doped PbO2 matrices, which retain the PbO2 structure upon doping (49–51). PbO2 films prepared by electrodeposition have been shown to yield mixtures of both orthorhombic (α) and tetragonal (β) polymorphs (52–54) (SI Appendix, Fig. S14); however, the similarity of Pb–O and Pb–Pb bond lengths for these two polymorphs (55–57) does not allow them to be distinguished by XAS. More insight into the nature of the host structure of NiPbOx and NiFePbOx films is offered by XPS spectra. The Pb 4f peaks shift toward higher binding energies with the addition of Ni and Fe into the lattice (Fig. 3A). These shifts are not the results of differences in applied potential as the Pb 4f and O 1s spectra of PbOx held at 1.45 and 2.00 V are virtually identical and they do not appear to correlate with film stability in acid. These results suggest that Pb oxidation state alone does not dictate Pb 4f peak positions, which may be influenced by distortion about Pb induced by metal ion doping.
The dominant peak at ∼530 eV and smaller peak at ∼532 eV in the PbOx O 1s spectra are attributed to lattice and hydroxyl oxygens, respectively (58). NiPbOx exhibits a more prominent hydroxyl peak than observed in NiFePbOx (Fig. 4B), in accordance with the greater stability of NiFePbOx in acid. We surmise that as the PbOx lattice becomes etched by acid, more edge sites are generated, resulting in an increase in hydroxyl peaks in the O 1s spectra. In support of this contention, the hydroxyl peak of NiFePbOx films becomes more prominent (SI Appendix, Fig. S10B) with operation of the film in acid over the course of 40 h.
Mechanism of Acid Dissolution in PbOx-Based OECs.
Although dissolution is expected for metal oxides in acid (NiOx FeOx), once the metal ions are embedded in an acid-stable PbOx matrix, stability is engendered for extended periods of time, after which the catalyst overpotential rises quickly as evidenced by the relatively sharp inflection point in the chronopotentiometry curves (Fig. 1). This sharp increase in operating potential under constant current conditions may reflect the exponential relationship between current and potential. Assuming that the current passed is the sum of contributions from the catalyst and the underlying FTO substrate, the following expression describes the total current:
[1] |
where j0(Cat) and j0(FTO) are the exchange-current densities for the catalyst film and FTO, respectively, mCat and mFTO are the Tafel slopes for the catalyst film and FTO, respectively, and η is the applied overpotential. In this regard, the exchange-current density of the catalyst can be used as a proxy for the number of intact active sites in the film.
If we assume that the current from FTO and the Tafel slope for the catalyst remain constant over the course of the experiment, the exchange-current density of the catalyst as a function of applied overpotential over the course of a constant-current electrolysis experiment is given by
[2] |
Using this equation, the potential vs. time curves obtained in our studies may be recast as exchange-current vs. time plots, which better illustrate the number of active sites in a given catalyst film over the course of electrolysis. Fig. 6 displays such a plot for a NiFePbOx film. Inspection of the exchange-current density as a function of time reveals a steady loss of active sites from the film over the course of electrolysis, until the activity of the catalyst drops below that of the underlying FTO substrate.
A catalyst dissolution mechanism in which active sites are steadily lost over the course of electrolysis is supported by ICP data; comparison of metal content in as-deposited films versus after dissolution (after the inflection point in V1mA) shows a dramatic reduction in Fe and Ni content (SI Appendix, Fig. S11). The dissolution of these metal centers indicates that, even when embedded into an acid-stable PbOx lattice, the 3d metal-oxide ligation sphere is not fully protected from protonation at the edge sites, which in turn exposes more edge sites for continued film dissolution. Such a dissolution mechanism is supported by the growth in hydroxyl oxygen peaks in the O 1s spectra of NiFePbOx films over operation of OER in acid. We note that accelerated metal leaching occurs from this class of oxidic metallate OER catalysts in neutral solution when they are held at open-circuit potential (59) as an applied electrochemical potential is needed to extend the lifetime of these catalysts via self-healing mechanisms (60). As we show here, the stability offered by self-healing is further augmented by the appropriate choice of a host lattice for catalytic active sites.
Conclusion
Metal oxides are notoriously unstable in nonbasic conditions, especially when employed as catalysts for OER. The four-electron oxidation of water to oxygen is accompanied by the release of four protons. In basic solution, the concentration of OH– is appreciable and the protons released from water splitting may be neutralized. However, in water at pH 7 or near-neutral conditions, the concentration of OH– is low and the metal oxide is the strongest base as reflected in the Lux classification of bases (61). Hence typical metal oxides are prone to corrosion by the leaching of metal ions and dissolution of the oxide. To overcome corrosion in water, we have developed self-healing catalysts that are able to self-assemble at applied potentials less than that needed for catalyst turnover (60). Solution pH provides a convenient handle for controlling the potential of these two processes, and as we have shown, may be exploited in the stabilization of catalyst in neutral and near-neutral water. However, at acidic pHs, self-healing is difficult to implement. Hence, new design approaches are needed for performing OEC in acid. To this end, we show here that template, acid-stable frameworks provide a viable milieu to extend the stability of metal oxides that otherwise corrode in acid. The mixed-metal-oxide design is bolstered by the flexibility with which one can incorporate disparate metal centers that serve as the 1) active center for oxygen evolution, 2) acid stabilizing framework, and 3) OER activity enhancers. To this end, we illustrate here that the high activity of oxidic Ni catalyst may be recapitulated in acid over appreciable periods of OEC when incorporated within an acid-stable PbOx matrix. In situ and ex situ spectroscopic X-ray techniques reveal that oxidic Ni-PbOx OER catalyst is a compact structure that mitigates attack by acid. Noting that practical electrolyzers require sustained OER activity for considerable operation times (62), our results offer a design element and an inroad for creating acid-stable catalysts that can promote water splitting at high activities.
Besides the practical aspect of enhanced stability, the ability to examine oxidic Ni:Fe vs. Ni OER in acid provides insight into the role of Fe in promoting OER by nickel oxide catalysts. Koper and coworkers have shown the importance of deprotonating γ-NiOOH in promoting OER (63). In native Ni oxy(hydroxides), this deprotonation can only occur under basic conditions. However, in near-neutral solutions (pH 9–11), the presence of the Lewis acidic Fe3+ may serve to increase the acidity of OHx (aqua/hydroxo) moieties that are coordinated to nickel, thereby facilitating OER. In contrast, in acidic solutions of pH = 2.5, the Lewis acidity of Fe3+ is abrogated and hence, as we report here, the presence of Fe3+ does not lead to enhancements in OER. The present work provides further support for the role of Fe as a Lewis acid in promoting OER. These results do not exclude the existence of multiple active sites, as has been proposed by others (40, 64), in which different active sites may promote catalysis in different pH regimes.
Data Availability.
All data needed to support the conclusions of this paper are included in the main text and SI Appendix.
Supplementary Material
Acknowledgments
Material is based on work supported under the Solar Photochemistry Program of the Chemical Sciences, Geosciences and Biosciences Division, Office of Basic Energy Sciences of the US Department of Energy Grant DE-SC0017619. We thank Joe Elias for assistance with XPS and Tuncay Ozel for help with SEM and Michael Huynh and David Gygi for helpful discussions. T.P.K. acknowledges support from a Graduate Research Fellowship from the NSF. R.G.H. acknowledges support from an Enrico Fermi Fellowship at Argonne National Laboratory (ANL). S.S.V acknowledges support from the Herchel Smith Graduate Fellowship in the Sciences. D.H. acknowledges support from a Joseph J. Katz Fellowship at ANL. L.X.C. acknowledges the support from Chemical, Biological and Geological Sciences, Basic Energy Sciences, Office of Science, Office of Basic Energy Sciences, under Contract DE-AC02-06CH11357. SEM and XPS were performed at Harvard University’s Center for Nanoscale Systems, a member of the National Nanotechnology Infrastructure Network, which is supported by the NSF under ECS-0335765. Use of beamline 12BM-B at the Advanced Photon Source at Argonne National Laboratory was supported by the US Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract DE-AC02-06CH11357.
Footnotes
The authors declare no competing interest.
This article contains supporting information online at https://www.pnas.org/lookup/suppl/doi:10.1073/pnas.2001529117/-/DCSupplemental.
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All data needed to support the conclusions of this paper are included in the main text and SI Appendix.