Metal-organic frameworks (MOFs) and metal nanoparticles are two classes of materials that have received considerable recent attention, each for controlling chemical reactivities, albeit in very different ways. Here, we report the growth of MOF shell layers surrounding aluminum nanocrystals (Al NCs), an Earth-abundant metal with energetic, plasmonic, and photocatalytic properties. The MOF shell growth proceeds by means of dissolution-and-growth chemistry that uses the intrinsic surface oxide of the NC to obtain the Al 3+ ions accommodated into the MOF nodes. Changes in the Al NC plasmon resonance provide an intrinsic optical probe of its dissolution and growth kinetics. This same chemistry enables a highly controlled oxidation of the Al NCs, providing a precise method for reducing NC size in a shape-preserving manner. The MOF shell encapsulation of the Al NCs results in increased efficiencies for plasmon-enhanced photocatalysis, which is observed for the hydrogen-deuterium exchange and reverse water-gas shift reactions.

Here, we investigate the bottom-up encapsulation of chemically synthesized Al NCs within a MOF layer. A MOF synthesis approach has been developed, where Al 3+ ions are etched from the surface oxide and are incorporated into the MOF framework as it is grown, enabling MOF encapsulating layers of varying thicknesses to be synthesized. With the removal of the Al 3+ ions from the surface, the surface oxide layer retreats further into the Al NC, resulting in a systematic and controlled reduction of Al NC size without changes in the NC shape. We demonstrate the utility of Al NC@MIL-53(Al) nanoparticles for photocatalysis, showing that the restricted diffusion of reactant species away from the substrate due to the presence of the MOF layer increases the photocatalytic reactivity of Al NCs toward hydrogen exchange and reverse water-gas shift (rWGS) reactions.

There have recently been increased efforts to identify Earth-abundant materials that may be possible substitutes for more precious metals in applications such as plasmonics and photocatalysis. The efforts toward the controlled growth of Earth-abundant plasmonic nanomaterials, such as aluminum ( 10 – 12 ), copper ( 13 ), titanium nitride ( 14 ), and other materials, have begun to shift focus to their photocatalytic properties. Beyond the noble and coinage metals, however, the oxidation of metallic nanoparticles is a common occurrence, and the presence of surface or bulk oxides markedly alters their inherent properties, chemical reactivities, and photocatalytic activities toward certain chemical reactions. In this regard, aluminum, the most abundant metal in Earth’s crust, is particularly intriguing. Historically, aluminum nanopowders in combination with oxidants have been studied extensively as a potent nanoenergetic material ( 15 ). However, more recent efforts have focused on their plasmonic properties, which can be obtained through precise synthesis methods and growth under highly pristine conditions ( 16 ). Because of the formation of a 2- to 4-nm passivating surface oxide that arrests further oxidation, aluminum nanocrystals (Al NCs) and nanostructures can be quite stable and useful for applications ranging from chemical sensing ( 17 , 18 ) to optoelectronic devices ( 19 ) to vibrant full-color displays ( 20 , 21 ) and even water desalination ( 22 ). Their role as plasmonically driven photocatalysts has been recently demonstrated, as photocatalysts themselves ( 23 ) and as plasmonic “antennas” when combined with catalytic nanoparticles and oxides in antenna-reactor complexes ( 24 , 25 ).

Metallic nanoparticles have been a major and ever-increasing research focus because of their enhanced reactivity relative to larger mesoscale and bulk phase materials ( 1 ). Over the past decade, much chemistry research has been concerned with the growth and reshaping of metallic nanoparticles and the inherent modifications of chemical reactivity that may result from changes in their size and shape ( 2 ). In addition, recent advances in photochemistry have relied on the collective electronic resonances (plasmons) of metallic nanoparticles to drive otherwise energetically unfavorable chemical reactions at temperatures and pressures far below those that typify conventional catalysis ( 3 – 5 ). In a parallel and equally dominant research focus, metal-organic frameworks (MOFs) have been synthesized and studied intensively for their ability to modify and enhance chemical reactivities ( 6 ). MOFs are complex three-dimensional (3D) networks with regular pores and channels that consist of crystalline lattices of metal cation centers (“nodes”) connected by multitopic organic linkers. Since MOFs have a range of intriguing properties including, but not limited to, exceptionally high porosity and surface area, they have been the subject of extensive studies for applications such as gas storage, chemical separations, and heterogeneous catalysis ( 7 ). The integration of noble metal nanoparticles within MOFs has been reported with concomitant enhancements of chemical and photocatalytic activities relative to either nanostructured material alone ( 8 , 9 ).

RESULTS AND DISCUSSION

Synthesis of Al NC@MOF An illustration of MOF layer growth around Al NC is shown in Fig. 1. This synthetic approach is inspired by naturally occurring pseudomorphic mineral replacement reactions, where the chemical structure of a mineral is changed without altering the spatial structure (26, 27). In this case, however, the dissolution of the Al NC surface oxide layer serves as a source of Al3+ for the backbone of the MOF, facilitating its growth and eliminating the need to introduce an additional metal precursor. In the presence of the organic linker, the kinetics of Al oxide layer dissolution is coupled to MOF layer growth, resulting in the formation of a uniform Al-based MOF shell layer around the Al core. Along with dissolution of the native oxide layer and MOF layer growth, the Al NC surface beneath the original native oxide is controllably oxidized, resulting in an overall reduction of the Al NC particle diameter (also illustrated in Fig. 1). This synthetic approach represents an opportunity to expand the surface chemistry of Al NCs and also provides a method for the highly controlled partial oxidation of Al NCs. Fig. 1 Synthesis of Al NC@MOF plasmonic heterostructure based on dissolution-and-growth. The controlled dissolution of the oxide layer through a one-pot mild hydrothermal strategy in the presence of the requisite organic linker leads to the formation of a uniform Al-based MOF shell around the Al core. In this scenario, the native oxide layer serves as a source of Al3+ for the backbone of the MOF. As the dissolution of Al3+ progresses, the surface oxide is regrown onto the Al NC, controllably etching the nanoparticle, but always maintains a surface oxide protecting the metallic Al core. Al NCs were first synthesized using a previously reported method (28). Transformation of the surface oxide layer into an Al-based MOF layer was accomplished through a one-pot hydrothermal strategy under a reaction temperature of 60°C in a mixed N,N′-dimethylformamide (DMF)/H 2 O solvent system (see Materials and Methods for synthetic details). Because of its well-studied coordination in conventional MOF synthesis, 1,4-benzenedicarboxylic acid (H 2 BDC) was chosen as the organic linker. Once the MOF is grown, the terephthalate (BDC) linker serves as a rigid spacer that connects the 1D parallel chains of AlO 6 octahedra and gives rise to the rhombic pores characteristic of this MOF, known as aluminum terephthalate [Al(OH)(bdc)] n MOF [also known as MIL-53(Al)] (29) (Fig. 2A and fig. S1). This MOF is of particular interest because of its excellent thermal and chemical stability. It exhibits dynamic shifts between its large rhombic pore and narrow trapezoidal pore configurations, termed breathing modes, depending on the presence and nature of guest molecules and environmental conditions (29). Fig. 2 Synthesis and characterization of Al NC@MIL-53(Al). (A) Schematic illustration of the structure of MIL-53(Al) grown around the Al core based on the dissolution-and-growth approach. Each aluminum center coordinates to two axial hydroxyl functionalities and four carboxylate units from linkers, sharing the coordination with the preceding and following Al centers in the chain. (B) Powder x-ray diffraction pattern of pristine Al NC, Al@MIL-53(Al) (activated for 4 hours at 150°C under vacuum), and simulated MIL-53(Al) in large-pore configuration. a.u., arbitrary units. (C) Transmission electron micrograph (TEM) image of single Al NC with the native oxide layer observable around the edge of the particle. (D) TEM image of single Al NC@MIL-53(Al). (E) Scanning electron micrograph (SEM) image of single Al NC. (F) SEM image of single Al NC@MIL-53(Al) showing a drastic change of the surface features compared with pristine Al NC. (G to J) High-angle annular dark-field scanning transmission electron micrograph (HAADF-STEM) image of (G) single Al NC@MIL-53(Al) and (H to J) surface rendering of Al NC@MIL-53(Al) in different orientations from electron tomography performed on the particle shown in (G). See movie S1. (K to N) HAADF-STEM image of a single Al NC@MIL-53(Al) particle (K) and energy-dispersive x-ray mapping of aluminum, carbon, and oxygen (L to N). Scale bars, 50 nm. Powder x-ray diffraction (PXRD) patterns of activated hybrid nanoparticles show multiple diffraction peaks in the range of 2θ = 5° to 35° and 2θ = 35° to 90°, corresponding to the crystalline lattice of the MIL-53(Al) and the Al NC core, respectively (Fig. 2B), as revealed by a comparison of experimental and simulated PXRD patterns of the MOF region. However, the full width at half maximum (FWHM) of the experimentally measured diffraction peaks in the MOF region is relatively broad. Considering the amorphous nature of the intrinsic surface oxide of aluminum, it is expected that the MOF shell layer that replicates the oxide layer structure exhibits small crystalline domains. Al crystallinity is well preserved during the MOF formation process: All indices corresponding to metallic face-centered cubic Al appear in the PXRD pattern of Al NC@MIL-53(Al) with relative intensities of the peaks remaining the same as for pristine Al NCs. This observation verifies that the dissolution-and-growth process preserves the crystalline structure of the parent NC during MOF formation. The characteristic vibrational bands of the MIL-53(Al) MOF formed around Al NCs were identified using Fourier transform infrared (FTIR) and Raman spectroscopy (fig. S2). Thermogravimetric (TGA) analysis showed that the MIL-53(Al) shell layer was thermally stable up to 450°C (fig. S3). Transmission electron micrographs (TEMs) show the formation of a conformal MOF shell surrounding the individual Al cores with no free MOF or remaining bare particles (Fig. 2, C and D, and fig. S4). Scanning electron micrographs (SEMs) reveal a drastic change in surface features from the typically smooth surface of Al NC to highly structured surfaces after MIL-53(Al) shell layer growth (Fig. 2, E and F, and fig. S5). The high-angle annular dark-field scanning transmission electron micrograph (HAADF-STEM) of an individual Al NC@MIL-53(Al) nanoparticle (Fig. 2G) shows a strong contrast between the bright Al core and the darker shell. Analysis of the 3D reconstruction of particle morphology using electron tomography shows the position of the Al NC within its MOF matrix, where the MOF shell uniformly encapsulates the plasmonic core with no holes or gaps; however, the fine surface features observable by scanning electron microscopy (Fig. 2F) were not reproduced in the tomographic reconstruction (Fig. 2, H to J, and movie S1). Elemental mapping of the Al core and MOF shell also supports the structural characterization of a conformal MOF shell layer surrounding an Al NC core (Fig. 2, K to N). In an alternate synthesis attempt, the previously established synthetic strategy for MIL-53(Al) was performed (29), where Al NCs were mixed with a metal nitrate precursor and the linker in an autoclave. Complete hydrothermal decomposition of the Al NCs was observed because of their inherent instability in hot aqueous solution (fig. S6). The apparent inability to synthesize Al NC@MIL-53(Al) by conventional MOF synthetic routes reinforces the importance of the dissolution-and-growth strategy pursued here. The dissolution-and-growth mechanism uses the 2- to 4-nm surface oxide layer that surrounds the Al NC core, which is independent of Al NC size. Therefore, under identical growth conditions, the MOF layer thicknesses should be uniform and independent of Al NC size as well. Figure 3 shows MIL-53(Al) shell layers grown around Al NCs varying in diameter from 50 to 150 nm, exhibiting dipolar plasmon resonances ranging from 350 to 680 nm in wavelength. The optical absorption of MIL-53(Al) is shown for comparison (Fig. 3A). Despite the consistent reduction in diameter of the Al NCs following MOF growth, an overall red shift of the localized surface plasmon resonance (LSPR) is observed for all particle sizes after MOF growth, which is dominated by the increased refractive index of the dielectric environment because of the growth of the MOF shell layer. Fig. 3 Al NC@MIL-53(Al) with tunable surface plasmon resonance. (A to D) Representative TEM images of Al NC@MIL-53(Al) with nominal Al core sizes of (A) 50 nm, (B) 85 nm, (C)110 nm, and (D)150 nm and their corresponding normalized extinction spectra before and after MIL-53(Al) growth. The extinction spectrum of the pure MIL-53(Al) is provided in (A). Scale bars, 50 nm. For particles larger than 100 nm, additional peaks appearing at wavelengths <550 nm correspond to the quadrupolar plasmon resonance. Interband absorption of Al appears at nominally 820 nm. (E) Experimental and theoretical scattering spectrum of bare and MOF-coated particles, showing narrowing of the dipolar plasmon linewidth as a result of MOF growth around Al NC. SEM images of the nanoparticles used to obtain these spectra are shown on the right. Scale bar, 100 nm. (F) FWHM and (G) quality factor (peak energy divided by FWHM) for the MOF-coated Al NCs compared to pristine Al NCs. Single-particle dark-field scattering measurements were also taken for bare Al NC and for similarly sized MOF-coated particles (Fig. 3E). For the bare Al NC, the scattering spectrum exhibits a pronounced dipolar mode around 3.3 eV and agrees very well with the calculated spectrum where the geometry of the particle is assumed to be spherical. The Al quadrupolar resonance around 5 eV lies outside the spectral window and cannot be seen. The MOF coating introduces substantial spectral changes. The quadrupolar and dipolar modes red-shift by around 1 eV and are now both visible in the spectrum. A pronounced narrowing of the dipolar plasmon linewidth is apparent. The calculated spectrum (modeling the MOF as a spherical shell of a refractive index of n = 1.5) shows the same spectral changes as the experiment. The slight disagreement for the intensity and energy of the quadrupolar resonance is most likely due to the particle having a nonspherical shape. Analysis of the spectra for a number of particles (Fig. 3, F and G) showed distinct improvements in the FWHM and corresponding quality factor (peak energy divided by FWHM) for the MOF-coated particles compared to bare Al. Theoretical analysis showed that this effect is primarily due to the reduced radiative damping due to the LSPR red shift but with the slight size reduction of the Al core also contributing (30).

Kinetic control and MOF growth mechanism The coupling between the kinetics of dissolution and growth can be modified by changing the pH of the initial reaction mixture. In nature, the dissolution of oxide minerals (known as chemical weathering) has been well studied in hydrogeochemical processes, where dissolution is influenced by pH and by concentration of dissolved ligands (31). In Al NC@MIL-53(Al) synthesis, adding increasing concentrations of acetic acid to the reaction mixture lowers the initial pH from ~4.1 to ~3.5 (in the presence of 30 mM acetic acid). This pH manipulation causes an increase in the rate of dissolution and also reduces the rate of MOF nucleation because of suppression of linker deprotonation. As the reaction proceeds, the pH of the solution gradually increases (fig. S7), increasing the concentration of the deprotonated linker, which can initiate MOF growth and inhibit further dissolution of the Al NC core. By exploiting the sensitivity of the plasmon resonance of the Al NC@MIL-53(Al) nanoparticle to its core size and its surrounding dielectric medium, we can monitor the pH-controlled kinetic balance of Al NC@MIL-53(Al) synthesis in detail (Fig. 4). Fig. 4 Controlling the kinetics of Al NC dissolution during MOF formation. (A) Monitoring the LSPR shift of the Al core as a function of time during the formation of the MIL-53(Al) MOF shell in the presence of various concentrations of acetic acid (HOAc) in the initial reaction mixture. The magnitude of the LSPR shift is divided into regions (i) and (ii) representing the dissolution and growth steps, respectively (see fig. S8 for the complete extinction spectra). (B) Representative TEM images of Al NC@MOF heterostructure formed in the absence of acetic acid (orange) and the presence of 5 mM (blue), 15 mM (red), and 30 mM (green) acetic acid. Addition of increasing quantities of acetic acid to the initial reaction mixture controllably increases the rate of dissolution of the oxide layer, causing a greater degree of Al core shrinkage and formation of a thicker and denser MOF shell. (C) Size distributions of pristine Al NC and Al core encapsulated in MOF grown in the presence of 30 mM acetic acid. The LSPR shifts that occur during synthesis, for varying concentrations of acetic acid, are monitored (Fig. 4A). The LSPR blue shift in region (i) suggests that the reaction is dominated by the kinetics of Al dissolution, whereas the LSPR red shift in region (ii) indicates that little or no further Al dissolution is occurring, but rather, indicates MOF nucleation and growth. The growth dynamics of the Al-based MOF was previously studied using surface-enhanced Raman spectroscopy (32) to probe the vibrational modes of the free organic linker and metalated linker within the MOF enclosure. In contrast, monitoring the LSPR shift of the Al core provides an in situ probe for a simultaneous kinetic study of both Al3+ formation (from oxide layer dissolution) and subsequent metalation of the linker and enables differentiation of the dissolution-and-growth process into its component steps. The magnitude of the initial LSPR blue shift increases with increasing acid concentration, indicating a greater degree of Al NC dissolution and a greater thickness of the MOF shell layer (Fig. 4B). The particle size distribution shows an ~30-nm average reduction of Al core diameter for MOFs grown in the presence of 30 mM acetic acid (Fig. 4C). This series of dissolution and growth studies indicates that this approach can serve as a method for controlled etching of Al NCs, providing a route for precise tuning of the plasmon energy of Al NCs to shorter wavelengths. In a control experiment in the absence of linker molecules, uncontrolled dissolution of Al NCs within the reaction time scale was observed (fig. S9). In contrast to acetic acid, the addition of sodium acetate to the reaction mixture inhibited MOF growth despite the higher concentration of free linker anion (fig. S10). To further elucidate the specific mechanism for MOF formation around Al NCs, we investigated the progress of Al NC@MIL-53(Al) growth by quenching aliquots of the reactant mixture over the course of the reaction. We have identified a four-step mechanism based on pseudomorphic replacement, where corresponding electron micrographs of the nanoparticles obtained throughout the reaction revealed changes to the surface morphology at each step (Fig. 5). Oxide dissolution is initiated by fast hydration of the surface oxide (Al 2 O 3 + H 2 O ➔ 2AlOOH), followed by a reaction between the newly generated aluminum oxyhydroxy [AlO(OH)] surface species and adsorbed H+ to release Al3+ at the interface in the form of a metal aqua complex (33). The fast coordination between the aluminum aqua complex ([Al(H 2 O) 6 ]3+) and the linker anion enriches the interface with the metal complex–linker species at a supersaturated concentration that promotes MOF crystal nucleation, followed by further growth. The drawing in Fig. 5D assumes a plausible MOF growth mechanism in a perpendicular manner, where 1D chains of the AlO(OH) extend perpendicular to the NC surface and are connected to each other via linker molecules (27, 32). Fig. 5 Proposed mechanism of MOF [MIL-53(Al)] formation around Al NCs. (A to D) Schematic depicting the proposed dissolution-and-growth mechanism and corresponding TEM images (below) of nanoparticles obtained at various stages [(A) 20 min, (B) 40 min, (C) 60 min, and (D) 80 min] showing progressive MOF formation. The particle surface remains visibly unchanged during hydration of the surface oxide layer to aluminum oxyhydroxy [Al 2 O 3 + H 2 O ➔ 2AlO(OH)]. The dissolution of AlO(OH) by reacting with adsorbed H+ generates an interface with a high concentration of the aluminum aqua complex ([Al(H 2 O) 6 ]3+) that then quickly coordinates with the linker molecule to form mono- or oligomers of the metal complex–linker species. Localized supersaturation of the solid/liquid interface with coordinated species promotes nucleation of the MOF crystal near the same dissolution site. The onset of the nucleation process after approximately 60 min of the reaction time is consistent with the onset of the LSPR red shift observed during MOF formation (orange dotted line in Fig. 4A). The nucleation process is followed by MOF layer growth that is nearly complete at 80 min into the reaction. We note that, because of thermodynamic equilibrium, the newly generated oxide layer is continuously reestablished while constantly dissolving to supply Al3+ for MOF growth. Scale bars, 50 nm. The dependence of the AlO(OH) dissolution on the adsorbed H+ is consistent with the effect of the initial pH of the reaction mixture on MOF formation kinetics (Fig. 4 and figs. S7 and S10) and indicates the characteristic of high-degree pseudomorphic replacement, in which the primary dissolution process needs to be a rate-limiting step compared to the secondary growth step (26). We suggest that, independent of its dissolution rate, the oxide layer is continuously reestablished because of the thermodynamic equilibrium between oxide thickness and metal-ion diffusion from the surface layer of the metal into an interstitial position of the oxide (34). As a result, the regenerated surface oxide remains sufficiently thin (2 to 4 nm) for the continuous hydration-dissolution of noticeable oxide quantities (up to 30-nm reduction of Al core size in Fig. 4), which otherwise may not be accessible for a thicker oxide layer (32).

Gas uptake and plasmonic photocatalysis Plasmonic metal nanoparticles have attracted significant attention for photocatalysis because of their capability to activate chemical transformations on their surfaces under illumination (35, 36). The plasmon resonant interaction of light with metallic nanoparticles leads to the generation of energetic hot carriers upon plasmon decay, which, along with photothermal heating, can drive otherwise energetically unfavorable chemical reactions. Recently, Al NCs have been demonstrated as an Earth-abundant, low-cost alternative to Ag and Au for plasmon-mediated photocatalysis (23). We have investigated Al NC@MIL-53(Al) nanoparticles for their gas uptake properties and to examine the effect of the MOF layer on their photocatalytic reactivity relative to pristine Al NCs (Fig. 6). The porosity of the MOF shell layers of the Al NC@MIL-53(Al) nanoparticles was confirmed and quantified by N 2 sorption (Fig. 6A) and CO 2 sorption (Fig. 6B) measurements (see fig. S11 for pore size distribution). The Al NC@MIL-53(Al) nanoparticle uptake follows a type II isotherm for N 2 sorption at 77 K, an indication of its microporous (rather than macroporous) nature (37). In contrast, the N 2 sorption isotherm on bare Al NCs follows type III behavior, characteristic of a nonporous surface (37). The gravimetric Brunauer-Emmett-Teller (BET) surface area increased from ~45 m2 g−1 for pristine Al NCs to ~371 m2 g−1 after MOF formation. The MIL-53 series of MOFs has been considered to be promising materials for CO 2 capture and storage (38). The low-pressure CO 2 sorption isotherm shows significant enhancement of CO 2 uptake capacity as a result of MOF growth (Fig. 6B). This enhancement originates from dipolar or quadrupolar interactions between CO 2 molecules and the hydroxyl groups (–OH) in the MIL-53(Al) framework (39). Fig. 6 Enhancing gas uptake and photocatalytic activity of Al NCs through MOF shell layer growth. (A) N 2 adsorption isotherm for Al NC@MIL-53(Al) and bare Al NCs measured at 77 K. STP, standard temperature and pressure. (B) Low-pressure CO 2 adsorption isotherm for Al NC@MIL-53(Al) and bare Al NC measured at 273 K. The solid and open symbols represent adsorption and desorption, respectively. (C) Photocatalytic reactivity of AlNC@MIL-53(Al) compared to pristine Al NC for the hydrogen-deuterium (HD) exchange reaction. (D) Photocatalytic reactivity of AlNC@MIL-53(Al) compared to pristine Al NC and pure MIL-53(Al) for the rWGS reaction under 300-mW white-light illumination. CO formation under illumination was detected when CO 2 and H 2 were both present. Illumination of the photocatalyst in an inert He atmosphere did not produce any measurable product, verifying that CO formation was not due to the decomposition of any organic contamination that may be present. GC, gas chromatography. The photocatalytic reactivity of the Al NC@MIL-53(Al) nanoparticles was characterized for two benchmark reactions of hydrogen dissociation and reduction of carbon dioxide in the rWGS reaction, where the Al NC@MIL-53(Al) nanoparticles outperform pristine Al NCs under visible light illumination (see fig. S12 for extinction spectrum of the photocatalysts and emission spectrum of the light source spectrum). The rate of hydrogen dissociation on Al NC@MIL-53(Al) nanoparticles as a function of visible light power under ambient conditions is significantly higher than that of pristine Al NCs without the MOF shell (Fig. 6C), particularly at higher illumination powers [the isotopic hydrogen exchange reaction H 2 + D 2 ➔ 2HD was used to monitor hydrogen dissociation (23)]. Enhancement of the photocatalytic activity was also observed for the rWGS reaction relative to pristine Al NC (Fig. 6D), consistent with our CO 2 adsorption results. Similar to our previous work on plasmon-induced hot carrier–driven rWGS, we observed an increased selectivity in product formation under illumination over the traditional thermally driven reaction (25). Photocatalytic rWGS yields selective CO formation in contrast to the formation of both CH 4 and CO in thermally driven processes (fig. S13). Using pure MIL-53 (without Al NCs) as a control substrate, although significantly higher MOF weight loading can be achieved compared to Al NC@MIL-53(Al) nanoparticles, no rWGS photocatalytic activity is observed. This observation confirms the role of the Al NC core as the active plasmonic component in photocatalysis, where the MOF shell provides an enriched adsorbate concentration near the surface of the Al NC core.