Open Access Article
Ariana
Serban
a,
Meng-Ting
Liu
b,
Nanjun
Chen
a,
Hao Ming
Chen
*b and
Xile
Hu
*a
aLaboratory of Inorganic Synthesis and Catalysis, Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne (EPFL) Lausanne CH-1015, Switzerland. E-mail: xile.hu@epfl.ch
bDepartment of Chemistry, National Taiwan University, Taipei, Taiwan
First published on 2nd December 2024
Anionic exchange membrane (AEM) water electrolyzers are emerging as a cost-effective technology for green hydrogen production. However, state-of-the-art AEM electrolyzers rely on platinum group metal (PGM) catalysts for the hydrogen evolution reaction (HER). Currently, PGM-free HER catalysts exhibit inadequate activity and stability at high current densities in electrolyzer environments. Here, we report a simple electrodeposition method for a self-supported Ni4Mo–MoOx catalyst. This catalyst exhibits remarkable HER activity, as demonstrated both in three-electrode cells as well as in prototype AEM electrolyzers. In particular, the catalyst enables AEM electrolyzers to operate stably at current densities as high as 3 A cm−2, which had not been reported for a non-PGM HER catalyst. The performance (2 V@3 A cm−2) is comparable to the benchmark Pt/C, whereas the stability is even higher. Characterization and particularly operando X-ray diffraction and absorption spectroscopy reveal that the catalyst is an unconventional tetragonal Ni4Mo with a D1a superlattice whose surface contains in situ formed MoOx species. The cooperative action of MoOx and Ni4Mo enhances the volmer step of HER, attributing to the superior activity.
Broader contextThis research contributes to the ongoing efforts to develop efficient and cost-effective catalysts for hydrogen production, crucial for advancing the viability of green hydrogen technologies. It addresses key challenges associated with PGM-free catalysts, offering a promising alternative that could facilitate the commercialization and widespread adoption of AEM water electrolyzers in sustainable energy applications. Additionally, the insights gained from the characterization techniques provide a valuable understanding of the catalyst's structure–property relationships, informing future catalyst design strategies.This work discusses advancements in anionic exchange membrane (AEM) water electrolyzers, focusing on the development of a novel catalyst for the hydrogen evolution reaction (HER) without relying on platinum group metals (PGMs). It highlights the limitations of current PGM-free catalysts, particularly in maintaining activity and stability at high current densities typical of electrolyzer environments. The study introduces a new self-supported Ni4Mo–MoOx catalyst fabricated via a simple electrodeposition method. The main findings indicate that this catalyst demonstrates exceptional HER activity, validated in both three-electrode cells and prototype AEM electrolyzers. Notably, the catalyst allows AEM electrolyzers to operate stably at high current densities of up to 3 A cm−2. Moreover, its performance at 2 V@3 A cm−2 rivals that of the benchmark Pt/C catalyst, while exhibiting even higher stability. Characterization techniques, including operando X-ray diffraction and absorption spectroscopy, provide insights into the catalyst's structure and composition. Specifically, it identifies the catalyst as an unconventional tetragonal Ni4Mo with a D1a superlattice, with surface features containing in situ formed MoOx species. The superior activity of the catalyst is attributed to the cooperative action of MoOx and Ni4Mo, while its high stability is linked to the strong adhesion resulting from the unique electrodeposition conditions employed during fabrication. |
This method's novelty lies in the composition of the electrodeposition bath and the utilization of high-current density for deposition. Unlike the well-established NiMo electrodeposition baths containing boric acid as a pH buffer13 or citric acid as a complexing agent,14 or methods that employ low concentrations of NH4Cl with NH3 for pH adjustments; our approach features high-concentration of NH4Cl as the sole supporting electrolyte without any pH adjustment.15 The deposition contained NiCl2 and (NH4)6Mo7O24 as sources of Ni and Mo. If NH4Cl is replaced by the same concentration of KCl under identical electrodeposition current and time, no deposition occurs; if NH4Cl is replaced by (NH4)2(SO4) using the same parameters, the resulting sample has much lower activity and falls off the electrode after one measurement (Fig. S3 and S4, ESI†). These results indicate the critical role of NH4Cl in the deposition. We identified Cl2 as a by-product in the deposition, which was attributed to the chlorine evolution reaction at the anode. The dissolution of Cl2 in the deposition bath would lead to a decrease in pH, which was indeed observed experimentally (Fig. S5, ESI†). Our deposition current densities are at least seven times higher than the conventional ones (e.g., 50–250 mA cm−2). The higher deposition current density in our method is a deliberate choice to achieve a more compact and thicker electrode structure. This is feasible because the conductivity of the electrodeposition bath is sufficiently high: 26 mS cm−1 for the NiMo-AS1 bath, compared to 5.55 mS cm−1 for the NiMo-citric bath and 7.36 mS cm−1 for the NiMo-boric acid bath. We could deposit the catalysts on other conducting substrates such as Ni foam and Ni felt. As references, we also prepared “conventional” NiMo catalysts using standard Ni plating baths reported in the literature,12,13 In these cases, NiMo-citric represents the catalyst deposited from a citric acid-containing bath, whereas NiMo-boric represents the catalyst deposited from a boric acid-containing bath.
| Sample name | η@ 0.1 A cm−2 (V) | η@ 1 A cm−2 (V) | Sample name | η@ 0.1 A cm−2 (V) | η@ 1 A cm−2 (V) |
|---|---|---|---|---|---|
| NiMo-AS1/Ni mesh | 0.04 | 0.19 | NiMo-AS1/C paper | 0.13 | n.d. |
| NiMo-citric/Ni mesh | 0.11 | 0.34 | NiMo-citric/C paper | 0.38 | n.d. |
| NiMo-boric/Ni mesh | 0.13 | 0.34 | NiMo-boric/C paper | 0.53 | n.d. |
| Ni mesh | 0.23 | 0.45 | Pt/C | 0.14 | n.d. |
| Pt mesh | 0.20 | 0.42 |
We also electrodeposited the catalysts on carbon paper because of applications in AEMWEs. In the measurements using a 3-electrode setup in 1 M KOH solutions, the C-supported catalysts exhibit generally lower activity than their Ni mesh-supported counterparts (compare Fig. 2A to Fig. 1A). For comparison among different catalysts, we used the overpotential at 0.1 A cm−2 (η@0.1 A cm−2). As shown in Fig. 2A, our NiMo-AS -activated catalyst has a η@0.1 A cm−2 of 0.13 V, which is much lower than those of NiMo-citric (0.38 V) and NiMo-boric (0.53 V). Compared to a Pt/C reference, the NiMo-AS1 is less active at low current densities (10–100 mA cm−2), but more active at high current densities, especially in the range of 150–400 mA cm−2 (Fig. 2A). We think this result might be understood by considering a high intrinsic activity of Pt/C over NiMo, which leads to a lower on-set overpotential. As the current densities go higher, mass transport becomes more important. It is possible that H2 release from the NiMo-AS1 is more facile than from Pt/C, leading to higher activity at the former. The roughness factor-averaged LSV data (Fig. 2B), and the mass-averaged LSV data (Fig. 2C) for the electrodeposited catalysts show that NiMo-AS1 is much more active than NiMo-citric and NiMo-boric catalysts.
We then used the C-supported catalysts as the cathode for AEMWEs. The setup of our prototypes has been described previously.16,17 In brief, a Branion AEM from NovaMea was used as the membrane, and a NiFe catalyst supported on Ni foam was used as the anode. The electrolyte was 1 M KOH for the anode, and the cathode was “dry”. The transient IV curves are shown in Fig. 3A. The AEMWE, having our NiMo-AS1 HER catalyst, exhibits a high performance, with a cell voltage of 1.75 V at 1 A cm−2. An analogous cell with a Pt/C cathode performs similarly at low current densities (>0.5 A cm−2). But at higher current densities, this cell has slightly higher cell voltages (1.81 V at 1 A cm−2) than the cell with our NiMo-AS1 cathode. By comparison, the NiMo-citric-containing AEMWE performs worse, giving a cell voltage of 1.88 V at 1 A cm−2. The NiMo-boric-containing AEMWE performs poorly, with a cell voltage of 2.37 V at 1 A cm−2. The trend observed in the current–voltage profiles of these AEMWEs is consistent with the activity trend observed in the 3-electrode settings (Fig. 1A and 2A).
We further tested these AEMWEs in long-term (potentiometric) electrolysis. A discrepancy was observed in the voltages of AEMWEs obtained from I–V (Fig. 3A) and potentiometric electrolysis experiments (Fig. 3B) as a result of the different time scales of the measurements. The AEMWE containing our NiMo-AS1 cathode operated stably at 1 A cm−2 for 150 hours, with a final cell voltage of 1.81 V. After an initial “activation” process of several hours, the voltage remains largely constant. When the benchmark precious catalyst Pt/C was used, the AEMWE could also be operated at 1 A cm−2 for 150 hours, with a final voltage of 1.77 V. The AEMWE containing the NiMo-citric catalyst had a final cell voltage of 2.1 V, 290 mV higher than that of our NiMo-AS1 catalyst. Furthermore, there is a noticeable degradation rate of 0.53 mV h−1. For the AEMWE with the NiMo-boric catalyst, the initial voltage spiked to 2.42 V before stabilizing at approximately 2.2 V at a current density of 1 A cm−2. However, the cell ultimately broke down after 100 hours of operation.
To further demonstrate the utility of our NiMo-AS1/C paper catalyst for even higher current density applications, we tested the AEMWEs at 3 A cm−2. The AEMWEs containing either the NiMo-AS1 catalyst or the Pt/C catalyst had very close performance: 1.96 V for Pt/C and 2.03 V for NiMo-AS1. Both cells can be stably operated for at least 100 hours at a cell voltage of about 2 V. After 100 h, the cell containing Pt/C showed voltage fluctuations compared to the NiMo-AS1-containing cell.
We also tested NiMo-AS1 catalysts deposited on Ni foam and Ni felt for AEMWEs. The former led to a cell voltage of around 1.8 V at 1 A cm−2, while the latter led to a cell voltage of about 1.76 V at 1 A cm−2 (Fig. S15, ESI†). These results indicate a similar performance of NiMo-AS1 catalysts in AEMWEs on different GDLs, although their activity appears to be different in LSV measurements.
:
1 Ni/Mo atomic ratio for NiMo-AS1 after activation (Fig. S18 and Table S4, ESI†). Scanning electron microscopy (SEM) measurements reveal that the NiMo-AS1 catalyst, when deposited under optimal conditions, achieves homogeneous coverage on both Ni mesh and carbon paper supports (Fig. 4A–F) as well as on Ni foam and Ni felt (Fig. S19, ESI†). Shorter deposition times and lower current densities resulted in partial coverage, whereas longer deposition times and higher current densities caused more visible cracks, indicating reduced adhesion (ESI† Fig. S20 and S21). After electrolysis at 1 A cm−2 for 1.5 hours, NiMo-AS1 on Ni mesh remained intact with only minor cracks (Fig. 4C). For NiMo-AS1 on C, the carbon fibers were initially fully covered by the catalyst (Fig. 4E). After electrolysis, a small number of fibers became exposed (Fig. 4F), likely due to the evolved gas bubbles. Among different catalysts, NiMo-AS1 formed the most compact layer on carbon paper, while the NiMo-citric and NiMo-boric catalysts did not cover the fibers (ESI† Fig. S16). After 150 hours at 3 A cm−2, morphological changes occurred for all carbon-supported catalysts. NiMo-AS1 and NiMo-citric remained on the C support, whereas NiMo-boric was partially detached (ESI† Fig. S17). EDX mapping confirmed a homogeneous distribution of nickel and molybdenum in all samples before and after electrolysis, with no phase segregation (ESI,† Fig. S16 and S17). As a reference, Pt/C on carbon paper also showed a substantial morphological change and suffered from Pt loss after electrolysis (ESI† Fig. S16 and S17).
Transmission electron microscopy (TEM) analyses of catalyst layers of NiMo-AS1 detached from the Ni mesh support show a nanosheet structure of the catalyst (Fig. S22, ESI†), which was transformed into a more layered structure after HER at 1 A cm−2 for 1.5 h (Fig. S22, ESI†), selected area electron diffraction (SAED) show that the NiMo-AS1 catalyst (Fig. S22, ESI†) after activation is polycrystalline. The most intense diffraction spots, with a d-spacing of 0.2, 0.16,0.12 and 0.11 nm, were attributed to (121), (101), (132) and (431) facets of a tetragonal Ni4Mo (Fig. S23 and S24, ESI†). Energy dispersive X-ray spectroscopy (EDX) mapping confirmed the uniform distribution of Ni and Mo in the catalyst, both in the as-prepared and activated forms (Fig. S25, ESI†).
To probe the influence of the temperature on the morphology of the NiMo-AS1 catalyst, we performed electrolysis at 22 °C, 40 °C, and 80 °C for 100 hours and analyzed the surface morphology using SEM with a secondary electron (SE) detector (Fig. S26, ESI†). After electrolysis at 24 °C, the catalyst surface remained relatively heterogeneous, with a mix of rounded particles and undefined structures, suggesting a limited reorganization at this temperature. After operation at 40 °C, the surface underwent a noticeable reorganization and became more homogeneous with a smoother and more uniform morphology. After operation at 80 °C, the catalyst surface acquired distinct layered microstructures. These results indicate substantial surface reconstruction driven by heating.
The X-ray photoelectron spectroscopy (XPS) data of the as-prepared and activated NiMo catalysts (Fig. S27–S29, ESI†), including NiMo-AS1, NiMo-citric, and NiMo-boric, all indicate the presence of Ni and Mo in various oxidation states (Ni: 0, 2, 3; Mo: 4, 6, and more). These data suggest that the surfaces of the catalysts contain various Ni and Mo oxide species, which could be intrinsic to the catalyst or could be formed at the surface of the catalysts due to oxidation during the sample preparation and transfer stages. Because of this complication, a detailed analysis of the XPS data is difficult. Nevertheless, the XPS data clearly show the increase in the percentage of Mo on the surface of our NiMo-AS1 after activation (Fig. S27, ESI†). Such an increase is not observed for the NiMo-citric and NiMo-boric catalysts.
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| Fig. 5 (A) Operando XRD pattern of NiMo-AS1. (B) Operando XRD pattern of NiMo-citric. (C) Operando XRD pattern of NiMo-boric. | ||
Operando X-ray absorption spectroscopy (XAS) measurements were further used to probe the chemical state and structure of the active sites during activation and operation. The operando Ni K-edge X-ray absorption near-edge structure (XANES) spectra and extended X-ray absorption fine structure (EXAFS) of all three samples remained similar during both the activation process and the HER process (Fig. 6 and Fig. S30, ESI†), indicating minimal changes in the Ni sites. The Ni K-edge XANES spectra and EXAFS spectra (Fig. 6 and Fig. S30A–C, ESI†) indicate that the as-deposited NiMo-AS1 and NiMo-citric catalysts have Ni metallic bulk species, whereas NiMo-boric contains mostly NiO species with the presence of both Ni–O and Ni–Ni paths (Fig. 6F). The chemical state of the Ni sites was determined from the first derivatives of the Ni K-edge XANES spectra (Fig. S31 and S32, ESI†). Notably, for NiMo-AS1, the Ni sites remained almost unchanged at a “negative” oxidation state of −0.25 during both the activation and the HER processes (Fig. S33A and S34A, ESI†). This result might be understood by considering charge transfer from Mo. Conversely, for NiMo-citric and NiMo-boric, the chemical state of the Ni sites remained almost unchanged oxidation states at 0 and +1.8, respectively, during both the activation process and the HER process (Fig. S33B, C and S34B, C, ESI†).
The operando Mo K-edge XANES of NiMo-AS1 and NiMo-boric indicates dynamic changes in the Mo sites, while NiMo-citric remained similar during both the activation process and the HER process. (Fig. 7A–C and Fig. S35, ESI†) The first derivatives of the Mo K-edge XANES spectra of NiMo-AS1 indicate that Mo sites reduced from approximately +1.5 to around +0.5 during the activation process and remained at approximately +0.5 during the HER process (Fig. S36A, S37A, S38A and S39A, ESI†). The operando Mo K-edge EXAFS spectra of NiMo-AS1 indicate the emergence of Mo–O bonds during the activation process, while the local structure of Mo centers remained similar during HER (Fig. S35D and S36D, ESI†). In contrast, the chemical state of Mo centers in NiMo-citric remained almost unchanged at an oxidation state of −0.5 during both the activation and the HER processes (Fig. S35B, S36B, S37B and S38B, ESI†). Additionally, no Mo–O bonds were formed during the activation and the HER process, which may be induced by the protection of citric acid (Fig. S34B and S35E, ESI†). As for NiMo-boric, the Mo centers were slightly reduced and remained almost stable during the HER process (Fig. S36C, S37C, S38C and S39C, ESI†). Furthermore, there were no Mo–Mo/Ni bonds observed in the Mo K-edge EXAFS spectra, indicating that the Mo sites in NiMo-boric were atomically dispersed with the presence of Mo–N/O/C path only (Fig. S35F, ESI†). A quantitative EXAFS analysis was further performed to characterize the coordination environment of NiMo-AS1 and NiMo-citric (Fig. S40–S55 and Table S5–S12, ESI†). In NiMo-AS1, the coordination number (CN) for Ni–Mo was approximately 1, while that for Mo–Ni was around 3. This result suggests a significant heteroatomic interaction between Ni and Mo, leading to a notable deviation from the ideal model of random distribution. Additionally, the total CNs for Ni–(Ni + Mo) was significantly lower than that of Ni foil, indicating a poor crystalline nature on the catalytic surface through the total-fluorescence-yield mode (see materials and methods). Notably, one can see that the interatomic distance for Mo–Ni is similar to those of Ni–Mo and Ni–Ni cases, which further supports the suggested charge transfer between Ni and Mo.
Furthermore, the CN of Mo–O in NiMo-AS1 increased from 0.5 to around 1.5 during the activation process, and the structure remained stable during the HER. The CN of Mo–Mo in NiMo-citric was around 2, while there were no Mo–Mo bonds observed in NiMo-AS1. After activation, Mo is reduced towards metallic, and according to EXAFS (Fig. 7), the CN of Mo–Ni increases by about 0.6 (see Table S6, ESI†) during activation. Moreover, the CN of Mo–O increases substantially, and the corresponding bond distance decreases by 0.07 Å in this process. In contrast, the EXAFS fitting results indicate the Mo species in NiMo-citric is metallic in nature even in the as-prepared sample; during activation and HER, the Mo species remain similar, while no Mo–O path can be revealed in this catalyst (Table S9–S12, ESI†).
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![]() | (2) |
![]() | (3) |
| 2H2 + NiMoO2 → NiMo + 2H2O | (4) |
As HER occurs, the local pH of the deposition bath increases so that precipitation of Ni and Mo oxides might occur, especially for a poorly buffered solution. Thus, the formation of NiMo oxides or hydroxides from the bath containing boric acid can be attributed to the latter’ poor buffering capacity. Such a problem can be circumvented by a complex agent such as citric acid that solubilizes the Ni and Mo precursors.23,24 For the deposition of our catalyst, NH4Cl plays a key role here in that the anodic Cl2 evolution and subsequent dissolution leads to a decrease, rather than an increase, in pH (Fig. S5, ESI†). This effect allows for a deposition current density to be an order of magnitude higher than previous methods. Moreover, NH4+ cation provides a better source of proton than water, which explains why KCl could not be used as the electrolyte.
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| Fig. 8 Schematic diagram of the surface re-organization of the catalyst during hydrogen evolution reaction. | ||
A more important parameter to compare for catalyst applications is the performance of devices using such catalysts. Indeed, our catalysts were designed for applications with AEMWEs in mind. Gratifyingly, comparing the device performance with state-of-the-art PGM-free catalysts demonstrates the superiority of our catalyst16,27–33-(Fig. 9). For this comparison, we focus on electrolysis data from relatively long-term operations (>100 hours) rather than those from transient IV measurements, as the latter does not reflect the steady-state performance of the systems.
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| Fig. 9 Comparison of the state-of-the-art PGM-free AEMWE cells. The numbers in the figure refer to the numbers of the references. | ||
The stable operation of our AEMWE at 3 A cm−2 is particularly noteworthy, as it had not been reported previously for any PGM-free AEMWEs. Our group recently reported that cathode ionomers can improve the performance of AEMWEs.16 Thus, appropriate ionomers might further improve the current AEMWEs using NiMo-AS1 as the HER catalyst. This objective is subject to future work.
We think the superior intrinsic activity of NiMo-AS1 might originate from its structure. Probably due to the D1a superlattice structure, our Ni4Mo pre-catalyst is subject to a re-organization in the activation process in which some bulk Mo atoms migrate to the surface to form MoOx clusters. Analogous Ni4Mo/MoOx assembly catalysts have been prepared by alternative methods34 such as growing Ni4Mo on MoOx nanosheet35 or by making NiMoO4 and subsequent annealing in a reductive atmosphere.26 Mechanistic studies, primarily based on DFT computations, suggest that the MoOx species facilitate the water dissociation to provide proton for the hydrogen adsorption on the Ni4Mo surface26,28,34 (the Volmer step, Fig. 10). In the absence of an oxide, the water dissociation in an alkaline medium is known to be difficult for metals. We expect a similar explanation for the superior activity of our catalyst described here.34
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| Fig. 10 Schematic diagram of synergetic catalysis of alloy–oxide interface structures, in which the molybdenum oxide promotes water dissociation, and the alloy accelerates hydrogen combination. | ||
000 eV) were conducted in total-fluorescence-yield (TFY) mode by the Lytle detector. The scan ranges for the Ni K-edge, and the Mo K-edge were 8133–8933 eV and 19
800–20
600 eV, respectively. The XAS data were calibrated using an E0 value of 8333.0 eV for Ni foil and 20
000.0 eV for Mo foil, referencing their respective first inflection points in absorption K-edge. The XAS data were analyzed using standard procedures, including background subtraction and edge height normalization. EXAFS spectra were obtained using the Fourier transform on k3-weighted oscillations to determine the local environment of the Ni and Mo atoms. The operando XRD measurements were conducted using a wavelength of 0.6889 Å (18 keV). The above operando measurements were performed at the 12B2 Taiwan beamline (SPring-8, Japan) of the National Synchrotron Radiation Research Center (NSRRC), operated at an 8.0 GeV storage ring with a constant current of ∼99.5 mA. A customized Teflon cell, which utilized Kapton tapes as an X-ray window, was employed for conducting operando measurements at ambient air/temperature in a 1.0 M KOH electrolyte. The sample electrodeposited on the carbon paper was used as the working electrode, while a graphite rod and Ag/AgCl in a 3 M KCl solution were employed as the counter and reference electrodes, respectively.
AEMWE assembly procedure: 40 μm-thick NovaMea's Branion AEMs with 1 mol% of 1,3,5- triphenylbenzene monomer (b-PTP-1, IEC = 2.81 mmol g−1) were used in this study for performance tests. The cathode PGM catalyst was Pt (weight fraction of 40%) supported on Vulcan XC-72R (Alfa Aesar HiSPEC 4000). The ink dispersions were sprayed onto Toray TGP-H-060 PTLs with PTFE wetproofing (weight fraction of 5%). The catalyst loadings were kept at 0.6 mgPt cm−2. The PGM-free self-supported NiFe-anode and NiMo-AS1 cathode were directly used in the AEMWE without any further treatment.
The membrane was soaked in 1 M KOH for 12 h prior to use and then the wet membrane was placed with OER and HER electrodes to prepare the PGM-free MEA. Subsequently, the MEAs were loaded into a 5 cm2 Dioxide Materials AEMWE hardware between two single-pass serpentine flow nickel plates. The MEA was sealed and compressed with 10 mil (270 μm) and 6 mil (160 μm) PTFE for anode and cathode, respectively, at 2.5 N m torque, resulting in 20–25% pinch. RND lab DC power supply was used to control the operating current density. The IV curves were recorded by holding each current density for 5 seconds and measuring the potential, starting from 0 A and increasing in increments of 0.3 A up to 2.3 A. A home-assembled temperature controller and sensor-controlled cell temperature at 80 °C. A Golander peristaltic pump controlled the electrolyte flow rate at 1 mL min−1.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ee04528a |
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