Engineering Heterostructures of Layered Double Hydroxides and Metal Nanoparticles for Plasmon-Enhanced Catalysis

: Artiﬁcially designed heterostructures formed by close conjunctions of plasmonic metal nanoparticles (PNPs) and non-plasmonic (2D) lamellar nanostructures are receiving extensive interest. The synergistic interactions of the nanounits induce the manifestation of localized surface plasmon resonance (LSPR) in plasmonic metals in the speciﬁc environment of the 2D-light absorbing matrix, impacting their potential in plasmon enhanced catalysis. Speciﬁcally, layered double hydroxides (LDH) with the advantages of their unique 2D-layered structure, tuned optical absorption, ease of preparation, composition diversity, and high surface area, have emerged as very promising candidates for obtaining versatile and robust catalysts. In this review, we cover the available PNPs/LDH heterostructures, from the most used noble-metals plasmonic of Au and Ag to the novel non-noble-metals plasmonic of Cu and Ni, mainly focusing on their synthesis strategies toward establishing a synergistic response in the coupled nanounits and relevant applications in plasmonic catalysis. First, the structure–properties relationship in LDH, establishing the desirable features of the 2D-layered matrix facilitating photocatalysis, is shortly described. Then, we address the recent research interests toward fabrication strategies for PNPs/support heterostructures as plasmonic catalysts. Next, we highlight the synthesis strategies for available PNPs/LDH heterostructures, how these are entangled with characteristics that enable the manifestation of the plasmon-induced charge separation effect (PICS), co-catalytic effect, or nanoantenna effect in plasmonic catalysis with applications in energy related and environmental photocatalysis. Finally, some perspectives on the challenges and future directions of PNPs/LDHs heterostructures to improve their performance as plasmonic catalysts are discussed.


Introduction Hybrid Plasmonic toward Optimized Photothermal-Photocatalytic Performances
Solar-to-chemical energy conversion by plasmon-driven photocatalysis is one of the sustainable approaches for obtaining intense electric fields, highly energetic electrons and local heating as tools to develop performant solutions to efficiently solve the environment pollution and improve the usage of solar energy. Among various promising routes, plasmonic hybrid nanocatalysts feature prominent solar driven surface plasmon resonance (SPR) [1]. SPR is related to the collective oscillations of the conduction electrons in metals and it can be classified into two modes: propagating surface plasmons (PSP) and localized surface plasmons (LSPR) [2].
By engineering the LSPR responses on a catalyst-molecule interface, a surface electronic state with an optimized energy can be created to selectively modulate solar-to-· mH 2 O, where the divalent M II and trivalent M III cations may be Mg 2+ , Zn 2+ , Ni 2+ , Cu 2+ , Al 3+ , Fe 3+ , etc., and the A n− can be almost any organic or inorganic anion [24,25]. LDHs may also be composed of M I or M IV , for example, Li + [26,27] or Ti 4+ [28,29], Sn 4+ [30,31], respectively. In such structures, the metallic cations are octahedrally coordinated to hydroxyl ions and form infinite layers of edge-shared MO 6   Considerable research efforts are continuously realized into the design of different LDH-type structures for photocatalytic purposes due to their unique properties, i.e., their great adsorption capacity, which may be extended to visible light absorption via compositional variation, well dispersed MO 6 units, and O-H surface bonds that can react with holes of valence bands to produce hydroxyl radicals, unique layered morphology and high specific surface area, possibility of transformation to mixed metal oxide special structures and unique memory effect features, and last but not least, the availability of cheap and scalable synthesis procedures. All these valuable features indicate their advantageous application as photocatalytic materials (in the form of non-calcined LDH, mixed metal oxides, or as supports in hybrid nano-assemblies) for various applications, such as in renewable energy production and storage (water splitting, CO 2 reduction, alcohol photo reforming, batteries) [12,[33][34][35] or pollutant degradation/removal in wastewater management [36][37][38][39][40][41][42][43].
LDH allow a very flexible choice in the nature of the metallic cations type to be inserted in the brucite-like sheets, resulting in binary, ternary, or multicomponent LDH, which together with the facile exchangeability of intercalated anions, facilitate their nanoscale tailoring for boosting the photocatalytic reactions. The cations in the MO 6 octahedral units are distributed in a uniform manner without clustering, offering a good metal dispersion, facilitating a wider separation of the electron-holes pairs, and thus, enhancing the photocatalytic activity by reducing the recombination. The combination of widely dispersed octahedral units sharing edges in a specific configuration in LDHs with variation of the nature of the metallic cations specifically identified as active in photocatalytic processes is of high importance. Various photocatalytic functionalities can be introduced by the isomorphous substitution of key metallic cations, as these can act as light absorbers and/or co-catalysts. In this context, the maximization of light harvesting (with extension to visible light) can be mentioned to generate sufficient energetic electrons and holes with high mobility, suppressing their bulk recombination and allowing sufficiently strong redox power to induce the targeted reactions. The effect is similar as the one achieved by coupling semiconductor nanoparticles having different band gap positions [44][45][46][47]. By tuning the LDH composition, the newly developed LDH materials may be regarded as nano assemblies of semiconductor nanoparticles where the advantageous layered network provides highly distributed metal cations in which the contact between the semiconductor active centers/sites is realized at the atomic level rather than at the particle level. This is of particular importance, as such highly uniformly dispersed catalytic active sites are not easily obtained in practice, where the control of homogeneity, consistency, and reproducibility is still a major issue, even at the laboratory scale.
Many research reports are demonstrating the importance of the mixed metal oxides derived from LDH structure as highly efficient photocatalysts as well as photocatalytic supports. The unique memory effect property is advantageously employed in heterostructuring of nanoparticles, e.g., of metals (PNPs) or oxides, stabilizing the PNPs onto the LDH surface or in the interlayer, controlling their morphology. The obtained heterostructures show the synergistic effects of the individual nano-units, with modified electronic structure, enhancement of light harvesting and improved photocatalytic efficiency [12,43].
As mentioned above, an important strategy of shifting the photoresponsive properties of the LDH-type materials and harvesting the visible light is to isomorphously insert key cations, e.g., Cu 2+ , Co 2+ , Ni 2+ , Fe 3+ , Cr 3+ or Y 3+ within the hydroxylic 2D [35,[46][47][48]. ZnCr-LDH is recognized for its potential of harvesting visible light irradiation [34,49]. Further, the hybridization of ZnCr-LDH with Au PNPs was reported to promote the degradation of gaseous volatile organic compounds and the nano-structuring of AuPNPs onto the LDH surface increased the photodegradation efficiency under visible light up to 83.6% [42]. Zhong-zhu Yang et al. describe that, in water splitting reactions, the transition metal-LDH or its nanocomposite is spatially separating the oxidation and reduction reaction sites due to the presence of both anions and cations in LDH which are both acting as reaction sites [47]. The tuning of the visible light absorption was also demonstrated for ternary LDHs composed of ZnCuAl or ZnCuGa [33] for which a red shift of their light absorption was observed. It was concluded that the insertion of Cu extended their absorption towards visible range based on the generation of an electronic state induced by Cu ions, leading to the narrowing of the LDH band gap. Furthermore, the same study, which focuses on the CO 2 conversion, reports that the insertion of Cu ions also influenced the selectivity towards methanol formation due to the fact that the Cu sites are also acting as binding sites for the CO 2 molecules, thus, interacting with the photogenerated electrons, protons and the Cu I /Cu II redox couple. As a consequence, the CO 2 molecules undergo a series of reduction reactions, forming CH 3 OH selectively. The narrow band gap is aligning with the redox level of CO 2 /CH 3 OH, which is favorable for the production of CH 3 OH under light irradiation. CoAl-LDHs manifest also a narrowed band gap with consequent absorption in visible range. By measuring the UV-Vis absorption spectrum of CoAl LDH, it was demonstrated that the light absorption lies in the visible range and the photocatalyst has an estimated band gap of 2.1 eV [33]. Such a photocatalyst was used in the conversion of very low concentrations of atmospheric CO 2 and water to CH 4 [50]. The improved photocatalytic conversion and CH 4 generation was based on (i) the ability of to capture the visible light, (ii) the enhanced CO 2 adsorption by the surface OH groups, and (iii) the unique effect of divalent Co. Bai et al. studied the effect of the various cations (Mg 2+ , Ni 2+ , Co 2+ , or Zn 2+ ) in the conversion of CO 2 under visible light irradiation and using the [Ru(bpy) 3 ]Cl 2 H 2 O as photosensitizer. Among the studied photocatalysts, the CoAl-LDH exhibited the highest CO conversion rate and H 2 production, and the NiAl-LDH showed the highest CH 4 production due to the selectivity of Ni towards CH 4 . These photocatalytic performances were associated with (i) the improved light absorption and capturing the maximum of visible light region, (ii) the defects on the photocatalyst surfaces promoting CO 2 adsorption, and (iii) well matched energy levels of the LDH with the photosensitizer molecules, thus, under light irradiation, the photogenerated charges are drained towards the LDH surface where they can efficiently react with the adsorbed CO 2 [51].
The anions in LDH were demonstrated as having a positive influence also due to the effect on the LDH light absorption range, enlargement of the specific surface area, and modulating the interlayer spacing among the LDH layers, which improves the photocatalytic performance by facilitating the essential reaction between the reactants and the photoinduced charge carriers [52,53]. It was demonstrated that the interlayer space within the LDH layers act as an active site when Cu is present, such as in the situation when the CO 3 2− anions were exchanged with [Cu(OH) 4 ] 2− anions. An increased CO 2 conversion with selective CH 3 OH formation was demonstrated when [Cu(OH) 4 ] 2− anions were intercalated, mainly assigned on the band gap narrowing and light absorption shifting after the intercalation of the [Cu(OH) 4 ] 2− anions [54]. Fluorine anions were found to enhance the photocatalytic activity based on the increased surface area of fluorinated LDH, while Cl − anions were demonstrated as acting as hole scavengers in a photocatalytic reduction of CO 2 using Cl intercalated NiAl-LDH, owing to the strong reducing character of Cl, − which is rapidly oxidized by holes, yielding HClO and selective formation of CO [55]. Intercalated organic anions, e.g., acetate anions, were also found to be advantageous in photocatalytic CO 2 conversion owing to the decomposition of the acetate anions absorbed on the LDH surface, which facilitates the electron transfer towards the CO 2 sites within the LDH [56].
In addition, the hydroxylated brucite-like layers are also advantageous for photocatalytic reactions. The surface-OH groups in LDH participate in the photocatalytic reactions in two different ways. First, the hydroxyl groups may be converted to hydroxyl radicals, which may be considered as the most effective reactive species responsible for photocatalysis [35,57]. Second, they may facilitate the formation of the ligand to metal charge transfer (LMCT) complexes on the surface of the semiconductor inorganic matrices, which favor the electron transfer and reduce the recombination, which promotes the process and enhances the photocatalytic efficiencies [58].

Plasmon Excitation in Metal Nanoparticles
Certain metal nanoparticles own unique optical properties that lead to the manifestation of SPR. Essentially, there are two experimental signatures of SPR: propagating surface plasmons (PSP) and localized surface plasmons (LSPR). Herein, we define metal plasmon nanoparticles as nanoparticles of metals that interact with photons through an excitation of LSPR. LSPR concentrates electromagnetic fields to the surfaces and its relaxation processes lead to convert photon energy to energetic charge carriers or heat, which can be harvested in photocatalysis [59]. It was revealed that LSPR response (intensity) is a function of both the nature of the metal and the size/shape of the nanoparticles [60]. However, most PNPs suffer from instability, aggregation behavior, and susceptibility to various "poisoning" issues, limiting their use in catalysis through deactivation and poor reusability [61]. To address these challenges, heterostructures of plasmonic metals stabilized on a support is an important approach. The support has the role to confine and stabilize the PNPs and, furthermore, to modulate the evolving plasmonic energy within the heterostructure [62]. Notably, representative progress in the field points to the high impact of the synthesis strategies in establishing the characteristics associated with LSPR and MSI (metal-support interaction) in hybrid nanostructures [19].
In recent years, nanosized Au, Ag and Cu received most of the attention because they exhibit resonant behavior when interacting with ultraviolet and visible (UV-Vis) photons in the condition that a large fraction of light consists of UV-Vis photons. Additionally, non-noble PNPs (e.g., Ni) are newly emerging as an alternative to noble-metal-based ones due to their advantages, such as earth-abundance, cost effectiveness and application capabilities, and until now, they were investigated to a much lesser extent. Therefore, herein, we shortly point out some recent achievements regarding the fabrication of noble (Au, Ag) and non-noble (Cu, Ni) plasmonic nanoparticles/support heterostructures.

Heterostructures of Noble Plasmonic Metals/Support
Since they were discovered, noble plasmonic nanoparticles have attracted the attention of researchers from all over the world due to their special optical properties. Most studies were conducted on AuPNPs, AgPNPs, due to their unique features, such as great stability, simplicity in chemical synthesis, and controllable surface modification [63].
Wang et al. fabricated 0D/2D Au/TiO 2 in a two-step process. First, TiO 2 was prepared by a hydrothermal method and further decorated with AuNPs using the in situ growth method (Figure 2a). They obtained square-shaped TiO 2 nanosheets decorated with 5 nm size AuNPs recognized in the heterojunction. This type of 0D/2D heterojunction is ideal for separating photogenerated charges [64]. One-step synthesis was used by Kunthakudee et al. [60] to synthesize Au/TiO 2 with a simple photo-deposition method. They mixed commercial TiO 2 with a HAuCl 4 solution and irradiated it with UV-visible light. During the irradiation, the temperature of the reaction was kept constant at 30 • C. A 0.5M NaOH solution was used to regulate the pH to the desired range (3.2-10). The obtained precipitate was separated by centrifugation, washed with water, and dried at 80 • C. The morphology showed semi-spherical AuNPs with a large average diameter of the particles. They proved that pH during the synthesis played a key role in tailoring the particle size of AuNPs, respectively, oxidation state. Thus, a decrease in the size of gold nanoparticles (from 34-77 nm to the range of 2.53-7.85 nm) was observed with increasing pH (from 3.2 to 10). Additionally, they found that at a lower pH (3.2), gold nanoparticles were deposited in metallic (Au0) and ionic (AuIII) states, while at higher pH (10) they were only in the metallic state [65]. Furthermore, Chang et al. reported the decoration of carbon nanorods (CN) and g-C 4 N 3 by AuNPs using the hydrothermal reduction method. Primarily, they obtained carbon nanorods by the solvothermal method. Furthermore, the CN was mixed with an aqueous solution comprising the gold precursor (HAuCl 4 ) and glucose and stirred for 30 min. The obtained mixture was hydrothermally treated in an autoclave at 120 • C for 12 h. As final steps, centrifugation, washing with water, and drying of the precipitate were performed. Au/g-C 4 N 3 was synthesized by the aforementioned method. The morphology after deposition showed a single CN decorated with approximately 13 nm diameter size AuNPs (Figure 2b). XPS measurements confirmed the presence of Au in the metallic state on the surface of CN and g-C 3 N 4 . UV-vis-NIR diffuse reflectance also confirmed the metallic state of AuNPs by the presence of the peak from 550 nm due to the LSPR effect of AuNPs [66]. An in situ method was used by Kashyap et al. to obtain AuNPs/CN nanosheets with high catalytic activity in Rhodamine B photodegradation. The CN nanosheets were obtained at 520 • C from urea with a 224 nm flake size. Spherical shaped AuNPs covering the CN nanosheets with a diameter 10.8 nm were noticed by HRTEM analysis. The XPS measurements revealed the presence of metallic Au 0 and Au δ+ species. Due to the -OH adsorbed groups that bind with the oxidized Au + species, the Au 2 O was formed [67]. A novel type of support for plasmonic metal nanoparticles widely used in photocatalysis are metal-organic frameworks (MOFs). In comparison to more conventional materials such as zeolites and clays, MOFs perform better because they are a revolutionary type of porous material with tunable pore size, improved specific surface area, and outstanding porosity [68]. Thus, Liang et al. reported the immobilization of AuNPs on MIL-100(Fe) by a facile photodeposition method. They obtained homogenously dispersed AuNPs on MIL-100(Fe) in the metallic state Au (0) with an average size diameter of 15 nm [69]. By the same method Cure et al. diffused ultra-small AuNPs (1 nm) into the MOFs (thiol-functionalized MOFs, including MIL-101 (Cr), MOF-808-SH) pores. They found out that thiol groups stabilize the AuNPs firmly into particular pores, maintaining their nucleation, and keep them apart. During the synthesis, AuNPs were completely reduced from Au(III) to Au(0) in the methanol solution, a fact that was confirmed by XPS analysis and the presence of the peak at 550 nm in the UV-vis spectrum due to the LSPR effect of AuNPs [70]. Silver nanoparticles deposited on different supports have demonstrated their potential in photocatalysis for more than three decades. A study by Stucchi et al. reported the preparation of Ag/TiO 2 by an ultrasound-irradiation-assisted reduction method with high photocatalytic activity in acetone degradation. AgNO 3 salt was used as the silver precursor and NaBH 4 as the reducing agent. Their findings showed an effect from ultrasound treatment on the silver nanoparticles morphology. The ultrasound treatment favors the agglomeration of AgNPs on the TiO 2 surface. Thus, not well distributed and different sizes of AgNPs (between 1 and 10 nm) were obtained. XPS analysis showed the formation of different species of Ag, such as metallic AgO and Ag 2 O [71]. Rabhi et al. doped TiO 2 with Ag using the sol-gel method as a photocatalyst in pharmaceutical effluent degradation. XRD results showed the formation of a tetragonal anatase-rutile phase and the Ag metallic phase. They noticed that increasing the concentration of Ag promotes the increasing of the rutile phase amount in the material [72]. Recently, a low-cost modified combustion method for synthesizing Ag/TiO 2 was reported by Cruz et al. They obtained a tetragonal rutile phase decorated with metallic AgNPs. TiO 2 with a granular morphology was obtained with a size ranging from 0.1µm to 1µm, as well as Ag with a size between 0.294 µm to 0.506 µm. The morphology of the obtained materials did not change after use in the photocatalytic degradation of methylene blue [73]. The deposition of AgNPs onto the g-C 3 N 4 were also reported. Chen et al. synthesized Ag/P-g-C 3 N 4 in a 2 step method. In the first step, P-g-C 3 N 4 was fabricated by thermal polymerization. Furthermore, the AgNPs were loaded by a photo-deposition route. The presence of (111), (220), and (311) planes show a cubic structure of AgNPs with a diameter size between 5 to 10 nm and nonuniformly distributed [74]. A more complex system was synthesized by Narkbuakaew et al. It included the formation of a heterojunction between g-C 3 N 4 and Ag/TiO 2 . The composite was obtained by mixing before producing g-C 3 N 4 (by hydrothermal method) with a H 2 SO 4 solution. Afterwards, Ag/TiO 2 was added to the aforementioned mixture. The slurry was centrifuged and dried at 60 • C. The TiO 2 particles were discovered to be embedded in g-C 3 N 4 sheets and Ag nanoparticles on the TiO 2 surface (Figure 3a). This facilitates photogenerated electron transportation, lowering the recombination process and boosting the photocatalytic properties [75]. For increasing the photocatalytic activity of MOF-based hybrid catalysts, loading with AgNPs also was developed recently. Guo et al. fabricated a MIL-101(Cr)-Ag metal-organic framework with application in CO 2 reduction. A chemical reduction of AgNO 3 by NaBH 4 was used for depositing AgNPs on the MOFs surface. They obtained well dispersed nanoparticles with an average size of 8 nm on different sizes of the MOFs support [76]. Another published paper reported the effect of synthesis method and parameters on photocatalytic degradation of organic pollutants by Ag-MOF hybrids. Thus, Hayati et al. used the loading method and sonochemical irradiation in order to synthesize Ag-MOF. Their findings have shown that Ag-MOFs nanostructures obtained by sonochemical irradiation present a small size and less agglomerated nanostructures with the best photocatalytic response [77]. Bimetallic Au-Ag deposited on semiconductors were also reported [78,79]. Yang et al. focused on tailoring the optical properties and synthesis method of Au-Ag/TiO 2 spheres through variation of Ag to Au ratios. They obtained a well-distributed binary of Au-Ag nanoparticles with a diameter size between 5 and 20 nm. Their optical response is shown in Figure 3b. After loading the noble metal Au-Ag nanoparticles, the absorption peak characteristic to TiO 2 suffered a red-shift from 390 nm to~460 nm. As a result, the ratio of Ag to Au in addition to the size of Ag or Au nanoparticles can be adjusted to influence the surface plasmon resonance absorption [80].

Heterostructures of Non-Noble Plasmonic Metals/Support
In the last few years, non-noble metals (Cu, Ni)-based plasmonic nanoarchitectures have attracted tremendous attention in the field of photocatalysis. Compared to the limited number of counterpart noble metals, the non-noble metals are considerably cheaper, highly available, and offer a broader spectral range of photoactivity, expanding the application area. Regarding the synthesis approaches, the discussion is similar to the many catalysts that require a specific nanoarrangement in terms of particles size, shape, or design (sandwich-like, nanotubes, nanosheets, nanoflakes, etc.) and the bottom-up method is by far preferred to the detriment of the top-down option. Furthermore, the non-noble metals are considerably more prone to form an oxide layer on the surface or even in the bulk regions, which may affect directly the photoresponse. In this regard, and taking into account the already extended focus on the preparation of noble metals plasmon nanoparticles (MeNPs), it is important for the future to draw the level between the advanced noble metal nanoparticles syntheses and, for the moment, primitive non-noble metal plasmons obtaining methods [9,81]. The current section targets the construction methodologies of photocatalysts consisting of non-noble metal nanoparticles (Cu, Ni), coupled with different inorganic or organic semiconductors or supports.
As one of the most studied materials in the photocatalysis field, TiO 2 represents a viable support for plasmonic MeNPs due to its outstanding long-known properties. Wei et al. designed an interesting heterostructure containing Cu NPs deposited on TiO 2 hollow spheres following a series of steps. First, carbon spheres (CS) were decorated with Cu NPs (Cu/CS) via a hydrothermal process. The resulted system was coated with TiO 2 using a controlled hydrolysis approach to obtain the Cu/CS@TiO 2 heterostructure. Finally, the Cu/CS@TiO 2 was calcined to remove the carbon spheres, and the catalyst was photoreduced. The electron microscopy investigations revealed that the resulting material was composed of Cu NPs of around 10 nm and TiO 2 hollow spheres with a diameter between 500-800 nm [82]. A simple and efficient Cu deposition on TiO 2 aerogels was employed by DeSario et al. involving a sol-gel method followed by a classical photodeposition of Cu NPs. Herein, the resulting composite revealed TiO 2 aerogels NPs of 10.3 ± 2.3 nm, while the Cu NPs, consisting of a mixture of Cu 0 , Cu 1+ , and a very small amount of Cu 2+ , have a relative diameter of 3.2 ± 0.7 nm [83]. Dai et al. built up a photocatalyst consisting of Cu 2 O octahedrons decorated with Cu NPs, to form an ohmic junction photocatalyst Cu@Cu 2 O. In their study, the synthesis of the Cu 2 O octahedrons was the first step, followed by an in situ chemical reduction with Cu + . The octahedra-like Cu 2 O crystals had diameters between 400 and 800 nm, while the tiny Cu NPs were anchored on the surface of the parental Cu 2 O [84].
Recently, Chen et al. assembled a unique doughnut-shaped heterostructure involving TiO 2-x /Cu/ZnO. In the first step, a TiO 2 /CuO support was obtained in the shape of doughnut via the spray pyrolysis technique. Next, different thickness layers of ZnO were encapsulated via atomic layer deposition (ALD) on TiO 2 /CuO, and the mixture was kept in a reducing atmosphere (Ar/H 2 ) at 500 • C for 4 h. The size of the doughnut varied in the range of a few µm with small Cu NPs deposited (few nm), while the ZnO layer could be varied due to the versatile method [85]. Organic materials may also be used as active photocatalytic supports coupled with plasmonic Cu NPs, as Xu et al. reported in their study. For the fabrication of the photocatalysts, the authors used a two-step thermal condensation pathway, which resulted in Cu nanocrystals (NCs) (2-5 nm) deposited on g-C 3 N 4 nanosheets [86]. Another promising support constructed is represented by MOF materials. The main reasons for their use in the photocatalytic field are directly related to the increased surface area, the ability to accurately tune the porosity network, and their chemical properties. Xiao et al. developed copper-mediated MOF photocatalysts, Cu@UiO-66 and Cu/Cu@UiO-66, as shown in Figure 4a. After following a classical method for the synthesis of UiO-66 MOF material, the authors used two different types of approaches to embed the CuNPs into and onto the MOFs, namely, the double-solvent approach (DSA) and advanced double-solvent approach (ADSA). Electron micrographs showed the formation of UiO-66 octahedrons (approx. 500 nm) and the presence of very small Cu NPs (1-10 nm) only for the samples where Cu loading was considerably increased [87]. Yu et al. focused their work on a very interesting system based on Cu single atoms (SAs) and Au-Cu bimetallic alloy NPs on TiO 2 . The preparation procedure followed a step-by-step photoreduction deposition approach and resulted in a nanoarchitecture ( Figure 4b) with AuNPs larger than 8 nm deposited on TiO 2 (Au/TiO 2 ) and a reduced number of Cu clusters (Cu/TiO 2 ), due to the fact that more Cu is present in the Cu-Au alloy forming Cu 0.8 Au 0.2 /TiO 2 [88]. Another attractive and efficient bimetallic alloy of Cu-Ag was integrated in a SiO 2 @S-doped graphitic carbon nitride (SC) core-shell design by Babu and collaborators. The obtained pathway involved a chain of syntheses, starting with the SiO 2 NPs, followed by the SiO 2 @AgCu nanoalloy, and concluding with the core-shell arrangement of SiO 2 @AgCu@S-doped C 3 N 4 . Regarding the morphology of the final material, SiO 2 particles of approx. 120 nm and layers of SC with a thickness between 3 to 5 nm were observed, while the Ag-Cu nanoalloy NPs diameter was determined to be around 1.3 nm [89]. In addition to Cu plasmonic NPs, remarkable results in environmental photocatalysis were observed also in the presence of Ni plasmons containing catalysts. As such, He et al. created a Ni-TiO 2 heterostructure following an adapted mediated nanosphere lithography method. The results showed a homogeneous layer of 200 nm TiO 2 deposited on silica nanospheres, on top of which another layer of 100 nm of Ni was attached. The size of the Ni-TiO 2 top layers with the SiO 2 nanosphere as a core can be tuned specifically to influence directly the optical properties [90]. Wang et al. developed a system consisting of black TiO 2 nanowire arrays, on top of which size-controlled NiNPs were deposited. The black TiO 2 was obtained via a hydrothermal approach, followed by the thermal hydrogen treatment, while the NiNPs were deposited via atomic layer deposition (ALD). Black titania nanowires characteristics were found to be around 25 nm in diameter and approximately 3.2 µm length. At the same time, NiNPs size could be controlled from the cycles of the ALD applied [91]. Tudu et al. designed another type of heterostructure consisting of a non-noble-metals bimetallic alloy, Cu-Ni, integrated in a TiO 2 thin film. The Cu-Ni alloy synthesis followed a classical hydrothermal approach, using hydrazine hydrate and NaOH solution as a reducing agent and alkali environment, respectively. In order to obtain the Cu-Ni/TiO 2 nanohybrid, the authors used a simple impregnation pathway by suspending the well-known P25 (TiO 2 ) in ethanol and mixing it with the Cu-Ni alloy suspension in ethanol. The textural investigations revealed the formation of an alloy-semiconductor heterojunction between spherical Cu-Ni NPs with a homogeneous particle size distribution (20-30 nm) and irregular TiO 2 crystals [92]. Kumar et al. had a similar idea to employ the synergistic effect of Cu and Ni in Cu-Ni alloy NPs dispersed in the same P25 (TiO 2 ) matrix. The synthesis procedure was reported to involve the co-impregnation of TiO 2 with Cu and Ni nitrates, with the formation of the Cu-Ni alloy during the photocatalytic tests as a result of the mild photoreduction conditions. The electron microscopy analysis revealed the intimate contact between Cu-Ni alloy NPs a few nm in size and irregularly shaped anatase/rutile nanocrystals [93].

Hybrid Plasmonics in Metal Nanoparticles/Layered Double Hydroxides Heterostructures
By virtue of the excellent adsorption capacity, tunable acidity-basicity [94] and the highly hydroxylated surface, the rigid and crystalline LDH sheets play multifarious roles in heterostructuring PNPs/LDH, including immobilization and stabilization of PNPs [95] while providing a unique interface-space confined in a 2-D porous matrix for controlling NPs spatial distribution [96]. On the other hand, serving as a support, the LDH matrix guarantees to stabilize low nuclearity nanospecies on its surface by minimizing atom diffusion, controlling the nanoparticle morphology, and modifying active nanometal electronic structure [97]. As previously mentioned, compared with the single component PNPs/LDHs, heterostructures show the advantages of the synergistic behavior of the coupled nano-units to effectively harvest light during catalytic processes. In this section, we will cover the basics and highlight some relevant studies that we believe illustrate the concept and possibilities of MeNP/LDHs as hybrid nanostructures from the viewpoint of the rational design and the synthesis strategies that will significantly determine their properties in plasmonic catalysis.

Heterostructures of Noble Plasmonic Metals/ Layered Double Hydroxides
Among a variety of noble metals, the research on heterogeneous catalysis based on AuNPs is one of the most relevant in the literature [98]. Firstly, Zhang et al. achieved the direct synthesis of AuNPs on MgAl-LDH with a homogeneous deposition-precipitation technique using urea as the precipitating agent [99] and HAuCl 4 as the gold precursor. They revealed that very small AuNPs (average size of 2-3 nm) were formed preferentially on the lateral (1010) faces of the LDH nanoplatelets. Varade and Haraguchi further reported a protocol regarding the synthesis of AuNPs/MgAl-LDH by exploiting the exfoliation of stacked LDH layers to provide positively charged nanosheets and further acting as a reducing agent of the NaAuCl 4 precursor [100]. Additionally, several recent publications reported AuNPs/LDH as active heterogeneous catalysts for various catalytic processes, such as: the synthesis of lactones from diols [101], the aerobic oxidation of alcohols under mild reaction conditions [102,103], coupling of nitroarenes to synthesize aromatic azo compounds [103], aqueous oxidation of 5-hydroxymethylfurfural into 2,5-furandicarboxylic acid under atmospheric oxygen [104], or deoxygenation of epoxides to alkenes using molecular hydrogen [105]. Although the aforementioned works reveal interesting applications in industrial catalysis, the amount of literature on the applications of AuNPs/LDH in plasmonic catalysis is very limited. Carja et al. reported a green preparation of AuNPs/Znbased LDH and tested their applications as plasmonic catalysts in hydrogen generation by water splitting under irradiation by solar light [12]. It is a green synthesis strategy in which AuNP/LDH is heterostructurally designed by exploiting the manifestation of the LDH "structural memory" property in an AuCl 3 aqueous solution, at room temperature. Notably, AuNPs were obtained directly on the surface of the LDH without using any additional chemical compound. During the clay reconstruction process, Cl − were taken by the LDH from AuCl 3 aqueous solution to reconstruct its interlayers, while Au 3+ were adsorbed organized as nanoparticles on the LDH surface [12]. By varying the LDH composition, noticeable effects from MSI for altering the plasmonic properties of AuNP/Zn-based LDH were noticed. Thus, UV-Vis and XPS results revealed that AuNPs oxidized faster for ZnCeLDH than for ZnAlLDH, leading to a larger steady-state population of positive Au + or Au 3+ and extended synergy between AuNPs and the LDH. This is important because it shows the impact of the LDH composition on harvesting the characteristics of plasmonic energy so as to modulate the manifestation of PICS in the indirect plasmonic catalysis. Next, some of us presented a detailed investigation on the oxidation state of AuNPs (as Au 0 , Au 3+ , as well as mixed Au 0 /Au 3+ ) and their SPR characteristics in AuNPs/ZnAlLDH hybrids by comparing the above-described calcination/reconstruction method and the impregnation/adsorption method [43]. First, we found that the synthesis procedure established both the nanomorphology and the characteristics of the plasmonic response in the designed heterostructures. Both syntheses have given rise to heterostructures where AuNPs smaller than 10 nm are highly dispersed on the larger nanoparticles of ZnAlLDH, with an average size of 110 nm, though the concentration of AuNPs on the large nanoparticles of ZnAlLDH increased when heterostructuring was realized by the calcination/reconstruction method (see Figure 5a-e). The UV-VIS results (Figure 5f), pointing to the red shift of the SPR peak from 539 nm to 547 nm, suggested the quantum size effect of AuNPs led to a lower-energy plasmonic near-field when AuNPs grew during the LDH reconstruction under UV-visible irradiation. We hypothesized that the special environment in which ZnAlLDH, reconstructed by the transformation of the mixed oxides, established tuned MSI that strongly impacted the plasmonic behavior of AuNPs/ZnAlLDH. Finally, EXAFS results provided further evidence for the synergistic behavior between AuNPs and ZnAlLDH. From this work it is clear that the electron transfer at the interface was faster when the conjunction between nanogold and ZnAlLDH was achieved by the calcination/reconstruction method when compared to the impregnation method. Thus, it is revealed that the synthesis procedure can be used, to a large extent, to establish the MSI and the plasmon induced electron transfer characteristics [106]. Another important example is the work of Zhu's research group, which revealed how the incorporation of phosphate anions (PO 4 3− ) and metal cations (such as Ga 3+ , Fe 3+ , and Zn 2+ ) in MgAlLDH established characteristics of AuNPs/MgAlLDH during the plasmonic catalysis for the reduction of nitroaromatics to azoxy-compounds under visible light irradiation [107]. The detailed procedure describing how MgAlLDH was first intercalated with PO 4 3− in the interlayers by the reconstruction method and after the junction between AuNPs and PO 4 3 /MgAlLDH was obtained by impregnation-reduction is shown in Figure 6. The authors claimed that the presence of PO 4 3− increased the charge redistribution and internal electric field inside the MgAlLDH and facilitated the electron transfer in the designed heterostructure. Furthermore, the introduction of Ga 3+ , Fe 3+ , and Zn 2+ in LDH positive layers resulted in a modified plasmonic response and increased catalytic performances. Similar to our findings, this validates that the LDH composition strongly impacts the plasmonic behavior in AuNPs/LDH and allows for performing chemical reactions beyond those for which only AuNPs play the role of catalytically active sites. Thus, this study revealed the entangled manifestation of a nanoantenna effect [20] by AuNPs and a co-catalytic effect by the substituted MgAlLDH in the plasmonic catalysis. Another interesting example in terms of the plasmonic hybridization of AuNPs/LDH was recently reported by Fu et al. [42] by studying visible light promoted degradation of gaseous volatile organic compounds catalyzed on AuNPs/ZnCrLDH. The catalysts were obtained in an aqueous medium containing ZnCrLDH, HAuCl 4 for gold precursor, and NaBH 4 as a reducing agent. AuNPs/ZnCrLDH nanomorphology was defined by almost spherical AuNPs with an average diameter of 8.6 nm well-dispersed on the LDH surface. In particular, Mott-Schottky measurements (Figure 7a) revealed a synergistic effect between AuNPs and ZnCrLDH, which could result in a major change of the band position compared to the bare LDH. Electrochemical impedance spectra (EIS) and Nyquist plots of ZnCrLDH and AuNPs/ZnCrLDH electrodes (Figure 7b) point out a suppression of the charge recombination generated by PICS. Furthermore, the absorbance at 680 nm vs. time for the open-circuited ZnCrLDH film electrode and AuNPs/ZnCrLDH in a N 2 -saturated acetonitrile ethylene glycol solution under visible light illumination before and after O 2 bubbling (Figure 7c) demonstrated the easier transfer of photoexcited electrons from ZnCrLDH to AuNPs due to the combined LSPR effect after coupling. Moreover, by monitoring the spectrum changes for the AuNPs/ZnCrLDH in the N 2 -saturated electrolyte without donor, before and after O 2 bubbled, under visible light irradiation (Figure 7d), it was found that AuNPs accepted electrons from ZnCrLDH. A dual electron transfer from AuNPs to Zn-CrLDH and the opposite transfer from ZnCrLDH to AuNPs should be noticed. Notably, this allows for the conceptualization of new designs of plasmonic heterostructures able to manifest both PICS and co-catalytic effects, thus, to favor the competition between direct and indirect plasmonic catalysis [108]. There were a number of recent reports concerning AgNPs/LDH heterostructures obtained by diverse synthetic strategies, including precipitation/thermal decomposition [38], anion-exchange precipitation method [109], and photoreduction [110] to obtain AgNPs/LDH heterostructures for catalysis. A good example is the work by Tonda and Jo, that describes Ag/NiAlLDH/g-C 3 N 4 composite for the efficient visible-light-driven photocatalytic removal of organic pollutants. The strategy to obtain Ag/NiAlLDH/g-C 3 N 4 composite was an in situ hydrothermal method, followed by photoreduction. In brief, LDH/CN composites were obtained by an in situ hydrothermal process. Thereafter, a series of Ag/NiLDH/C 3 N 4 with 1 wt% Ag and 5, 10, 15, and 20 wt% LDH to C 3 N 4 were obtained through the adsorption of AgNPs and their subsequent photoreduction using methanol as a hole [110]. The results of the transient photocurrent ( Figure 8a) and electrochemical impedance spectroscopy (EIS) measurements (Figure 8b) validated the transfer of photogenerated charge carriers within the nanocomposite system and the charge carrier separation efficiency. By taking advantage of better transfer efficiency of photoinduced charge carriers AgNPs/LDH/CN achieved a more effective charge separation compared to Ag/CN and LDH/CN. UV-vis analysis (Figure 8c) pointed out that the presence of AgNPs improved the light absorption over the whole wavelength regions and the intensity of the plasmonic response is a function of the silver content. Additionally, the junction between AgNPs and LDH/CN strongly decreased the intensity of photoluminescence (PL) spectra, as indicated in Figure 8d, revealing a mixing of the electronic states of the coupled components able to generate strong MSI characteristics between the plasmonic AgNPs and NiAlLDH/CN. This impacted both the electron-hole separation and the transfer of photogenerated charge carriers [111] between the three-component heterojunction system and established a lower recombination probability for photoinduced electrons and holes. Furthermore, a synergistic response in AgNPs/LDH was reported by Gilea et al. [37]. Specifically, we described AgNP/ZnAlLDH and AgNP/MgAlLDH as nanostructured assemblies that were synthesized in an aqueous solution, at room temperature, by exploiting the structural reconstruction of the calcined ZnAlLDH/MgAlLDH in the solution of Ag 2 SO 4 . The SPR features were effective to promote the behavior of AgNPs as both the light harvesting unit and the catalytic component for the process of phenol photodegradation from aqueous solutions, as shown in the next section. Lestari et al. [36] reported the synthesis of AgNPs/ZnAlLDH by the intercalation of AgNPs in the interlayer space of LDH exfoliated by dodecyl sulfate anions. Similarly, the excellent activity for phenol photodegradation in the aqueous solution was attributed to the manifestation of PICS during the electron donation from the plasmon-excited AgNPs to the conduction band of the ZnAlLDH semiconductor. The choice to combine the multiplasmonic response arising from different metallic plasmonic nanoparticles, via LSPR, might enable expansion of nanoplasmonics from the visible and near-infrared range toward the ultraviolet range. Thus, support tuning strategies to synthesize multiplasmonic catalysts are strongly required for the ultimate performance in hybrid catalysis. Recently, we studied in detail the plasmonic responses of PtNPs/LDH and PtNPs-AgNPs/LDHs heterostructures, obtained by the calcination reconstruction strategy, for the photocatalytic degradation of p-nitrophenol [40]. The role of the chemical composition of the LDH, as that partially defines the starting point for MSI, was analyzed by following the partial substitution of Zn 2+ by Fe 2+ in the composition of the PtNPs-AgNPs/LDH. The significant increase in the photoluminescence signal for Pt-AgNPs/ZnFeAl, as compared to Pt-AgNPs/ZnAl, indicated a retard recombination of electrons-holes in Pt-AgNPs/ZnAl and further validated the active role of the LDH composition to establish an effective electronic coupling and to inhibit the recombination of photogenerated charge carriers. In terms of light absorption properties, multiplasmonic Pt-AgNPs resulted in an extended SPR response in the visible and infrared regimes of the electromagnetic spectrum and improved the caption of the photogenerated electrons, unfolding the reasons for the superior catalytic activity. Similarly, Sahoo et al. reported that the multiplasmonic response of the AuNPs-PdNPs/ZnCrLDH/MCM-41 heterostructure was different from those of single AuNPs and PdNPs [112].

Heterostructures of Non-Noble Plasmonic Metals/Layered Double Hydroxides
While extensive reports exist on plasmonic catalysts based on noble metals nanoparticles, information about non-noble metals PNPs/LDH nanostructures remains scarce [81]. However, compared to noble-metal based plasmonic NPs the non-noble analogues are less expensive and might exhibit comparable performances to convert light energy by heterogeneous catalysis [113]. However, to date, few studies exist regarding the plasmonic properties of heterostructures of non-noble plasmonic metals/layered double hydroxides and their applications. CuNPs are just starting to be explored in plasmonic catalysis [61]. To obtain CuNPs/LDH heterostructures, Ma et al. reported a reduction procedure by using MgCuAlLDH and ascorbic acid for the reduction of copper [114]. By taking advantage of the tuned copper content of MgCuAlLDH, they obtained a broad size range of Cu 2 O nanoparticles highly dispersed on MgAlLDH. Furthermore, XRD, TEM, and XPS results disclosed a close conjunction of Cu 2 O nanoparticles with MgAlLDH that promoted their photocatalytic behavior under visible light while degrading orange II from water. To investigate the plasmonic optical responses in CuNPs/LDH heterostructures, some of us obtained CuNPs/ZnAlLDH and CuNPs/MgAlLDH heterostructures as active photocatalysts for the degradation of the industrial dye Nylosan Navy (Clariant Produkte) by irradiation of both Vis and UV light [115]. CuNPs/LDH nanoarchitectonics were synthesized by a simple and cost effective method based on the formation of nanoparticles of CuO on the surface of the eco-friendly clay during the structural reconstruction of the layered LDHs matrix in the aqueous solution of Cu(OAc) 2 . The derived solid solutions were obtained by calcination of CuNP/LDH at 750 • C. Investigations into the optical properties demonstrated a synergistic response between CuNPs and the LDH, while results from the optical direct band gap (Eg) values of the samples revealed narrow band gap values (3.34 eV for Cu/MgLDH, 3.21 eV for Cu/ZnLDH that decreased to 2.1 and 1.47 eV after the calcination). This is likely to promote plasmonic capabilities and disclose the semiconductor characteristics, while the electron transfer across the dye-semiconductor interface was found to increase the charge carrier lifetime and evidence the co-catalytic effect. To combine multiplasmonic responses for mitigating the limited visible light absorption in catalysis, the fabrication of Au-CuNPs/MgAlLDH catalysts was achieved by the impregnation-reduction method, by using HAuCl 4 and Cu(NO 3 ) 2 as precursors and NaBH 4 as a reduction agent [116]. Importantly, the resulting Au-CuNPs/MgAlLDH showed better performances in the oxidative esterification of benzyl alcohol with methanol in the presence of molecular oxygen to prepare methyl benzoate under visible-light irradiation in comparison to single plasmonic components, AuNPs/MgAlLDH and CuNPs/MgAlLDH, respectively. XPS results disclosed that the junction between Au with Cu led to electrons preferentially transferring from Au to Cu and facilitated the successful reduction of the oxidized surface Cu. Although the impact of MgAlLDH composition in the catalytic process is clearly demonstrated, the extent to which the electrons are transferred between the LDH and the plasmonic NPs by manifesting PICS and/or co-catalytic effect is not studied in this work.
The construction of NiNPs/LDH heterostructures was further explored as an effective means for obtaining an extended response in plasmonic catalysis. Plasmonic NiNPs display a localized yet tunable SPR in the UV−vis-NIR regions and offer the perspective in synthesizing highly active catalysts [117], although the exploitation of their plasmonic features still remains a pressing challenge and the amount of literature on the synthesis of NiNPs/LDH heterostructures is limited. Carja et al. developed heterostructures of NiNPs/MgAlLDH and NiNPs/MgFeLDH by a calcination-reconstruction method [118]. In an aqueous medium, at room temperature, NiNPs within the size range up to ca. 10 nm were highly dispersed on the surface of MgAlLDH and MgFeLDH by the mediated reconstruction in NiSO 4 ·7H 2 O solution. The SPR response of NiNPs is synergistically combined with the optical features of the LDH support. In 2021, Li et al. reported highly dispersed metallic NiNPs/NiAlLDH [119]. The specificity of the preparation method was assigned to the formation of NiNPs through the rationally designed mild liquid reduction method, described in Figure 9a. The XRD (Figure 9b) and HRTEM results clearly indicated the structural characteristics of the joined NiNPs and NiAlLDH nanounits with the NiNPs average size of~10 nm. Ni/NiAlLDH, obtained after 12 h reductions, exhibited obvious absorption across the entire solar spectrum (220-2000 nm) due to the surface plasmon absorption of metallic Ni. As revealed in Figure 9c, UV-vis-IR absorption results showed a wide SPR response defined by the absorption band at 645-710 nm due to the 3A2g(F)3T1g(F) transition, attributed to the spin-orbit coupling of nanosized Ni [120]. As a result, the plasmonic enhancement for Ni/NiAlLDH was strongly enhanced when compared to NiAlLDH for the wavelength range higher than 500 nm.

Metals/Layered Double Hydroxides Heterostructures for Applications in Plasmonic Catalysis
Mikami et al. reported the degradation of a toxic organic compound (phenol) from an aqueous solution by Au/ZnLDHs under solar light irradiation synthesized by the reconstruction and impregnation method. The parent LDH showed 7.6% of phenol degradation, while after gold deposition, the efficiency of the photocatalysts reached complete decomposition. The best catalyst was found to be reconstructed under solar light irradiation (Au/Zn 2 Al-Rec-3-Light). Samples synthesized by the reconstruction method showed a better photocatalytic activity compared with the one obtained by the impregnation method. As well, two different degradation pathways were noticed. An indirect ring opening process (through the formation of p-benzoquinone) describes the degradation by reconstructed materials and both indirect and direct opening ring processes (through the formation of catechol, o-benzoquinone, and then muconic acid) by impregnated materials. A key role in the photodegradation process had the oxidation state of gold nanoparticles (Au 0 , Au 3+ , and mixture Au 0 /Au 3+ ) deposited on the layered double hydroxide surface. Therefore, in order to achieve O 2 reduction, the fast electron transfer from LDH to Au sites was influenced by the interface of the Au 2 O 3 phase between metallic Au 0 and LDH. Since Au 0 NPs were not very well incorporated into the impregnated sample surface, it caused a slower electron transfer at the interface and a reduced charge separation efficiency. This study also revealed that increasing the Au nanoparticle's dimension and SPR intensity had no effect on the photocatalytic efficiency. Furthermore, a correlation between the surface of the catalyst and efficiency could not be found. The best catalyst (Au/Zn 2 Al-Rec-3-Light) proved to have good stability after five cycles of reusing. A minor decrease in efficiency of 30% was noticed. An approximately 10% increase in photocatalytic activity was observed after irradiation of the recovered catalyst after reuse. This can be explained by charge transfers between AuNPs and LDH produced under irradiation [43].
AuNPs/LDH showed good performance in the photocatalytic water splitting process. A study by Carja et al. reported Au/ZnAlLDH and Au/ZnCeAlLDH with high H 2 production from water splitting. They underlined the impact of the LDH composition and AuNPs dimension in photocatalytic H 2 generation. Thus, by adding Ce into the LDH composition the hydrogen production increased even though almost the same amount of gold was deposited on ZnAlLDH and ZnCeAlLDH. Calcined samples exhibited lower photocatalytic efficiency due to an increase in the size of AuNPs, causing a weak interaction between the metal nanoparticles with the support (SMSI). Another important factor is the distribution of the metallic (A 0 ) and cationic gold ( + and 3+ ) on the surface. Since the Au NPs introduce electrons into the LDH's conduction band, there ought to be an abundance of positive charge-density Au atoms. The presence of Ce from the LDH matrix promotes the electron injection, which increases the steady-state population of positive Au ( + or 3 + ) atoms in the material. Therefore, the deposited gold is oxidized more quickly throughout the photocatalytic process [12].
Xiao et al. investigated the reduction of nitroaromatics (nitrobenzene) to azoxy-compounds (azoxybenzene) by Au/LDH heterostructures under visible light irradiation. They tailored the hydrotalcite (HT) support by adding phosphate (PO 4 3− ) and metal ions M (such as Ga 3+ , Fe 3+ , and Zn 2+ ) in order to prevent the production of azo-and aniline compounds. Compared to the M-HT, PO 4 3-HT, and HT supports, Au/PO 4 3− -M-HT were the most effective photocatalysts, especially Au/PO 4 3− -Ga 3+ -HT. It showed good selectivity for azoxy compounds and high conversion. Reusing tests of five cycles for the best catalyst without any changes in activity proved good stability in this process. Furthermore, they explored the influence of light irradiation at different wavelength ranges by using block filters. It was noticed that conversion decreased for the wavelengths below 550 nm and 600 nm, while the range of 490-600 nm overlaps with the LSPR of gold nanoparticles, suggesting an antenna effect in AuNPs. The influence of light intensity and temperature of the reaction was also explored. The conversion increased linearly with the increase in temperature and light intensity until 0.7 W/cm 2 ; afterward, it increased non-linearly with the light intensity (Figure 10a). In order to obtain a full conversion, it was necessary to increase the temperature to 50 • C and the light intensity to 0.9 W/cm 2 . The electron transfer mechanism from Figure 10b shows the transfer of the light excited electrons into the conduction band of the support in order to create a positive charge density of AuNPs and to start the reaction. Additionally, PO 4 3− can also contribute to the electron transfer due to an increase in charge distribution. In conclusion, the reduction of nitrobenzene to nitrosobenzene (step 1) is possibly due to the energy generated by light-exited electrons of gold nanoparticles that activate the N-O bond. Furthermore, nitrosobenzene transforms very fast in phenylhydroxylamine, which can couple with nitrosobenzene and form the azoxy compound [107].
Volatile organic compounds (VOCs) were also removed by the photocatalytic process using heterostructures with AuNPs and LDH. These compounds are very toxic, mutagenic, and carcinogenic. Fu et al. reported the photocatalytic degradation of o-xylene by ZnCrLDH and Au/ZnCrLDH, as well as the influence of some factors, such as catalyst dosage, concentration of the pollutant, the temperature of the reaction, light intensity, and relative humidity. This study pointed to an increase in the photocatalytic efficiency after increasing the amount of gold deposited on the LDH surface and a decrease in the removal rate after the increase in the concentration of o-xylene. Furthermore, a study on the effect of the catalyst dosage, radiation intensity, and temperature of the reaction showed an increase in the removal rate with the increase in these parameters. As in the study carried out by Xiao, photocatalytic tests were carried out at different wavelengths range. In this case, they noticed that between 500-600 nm Au/ZnCrLDH showed the best efficiency due to the LSPR of gold nanoparticles. The photocatalytic mechanism can be described as follows: to avoid the recombination of e − -h + , gold nanoparticles deposited on the surface can serve as an acceptor of e − from the LDH support. In this way, holes would receive more opportunities to act individually for gaseous o-xylene photodegradation so that more electrons and holes may participate in the production of hydroxyl radicals. Because of this, Au supporting can significantly improve the photocatalytic performance of LDHs [42]. Silver decorated layered double hydroxides have also attracted the attention of scientists in past years for use as photocatalysts. Thus, only a few examples will be further discussed. Tonda and Jo studied the photocatalytic efficiency of Ag/LDH/g-C 3 N 4 nanocomposites in the degradation of Rhodamine B and 4-chlorophenol. For this study, different amounts of NiAlLDH (5, 10, 15, and 20%) were used for the synthesis of LDH/g-C 3 N 4 and 1% Ag for the decoration of LDH/g-C 3 N 4 . The best results in degradation of both RhB and 4-CP were obtained on Ag/LDH/g-C 3 N 4 with 15%LDH. This catalyst was recovered and reused in another five photocatalytic cycles (Figure 11a). It showed good stability in this reaction due to the charge transfer among CN and LDH, also the ability of AgNPs to effectively capture electrons. The proposed mechanism shown in Figure 11b shows the migration of the electrons from the CB of CN to CB of LDH excited by solar light irradiation. Furthermore, the charge separation forms due to the displacement of the holes from the band VB of LDH to the VB of CN. AgNPs from the surface act as electron traps and capture the electron from the CB of LDH and CN. The loaded AgNPs and the interface between the CN and LDH prevent the recombination of the charged carriers. As a next step, electrons from the AgNPs surface reduce dissolved oxygen in O 2 ·− species, followed by its conversion in ·OH. The generated O 2 − , ·OH species combined with photogenerated holes degrades pollutants such as RhB and 4-CP [110]. The photodegradation of antibiotics such as tetracycline (TC) by silver decorated ZnAlLDH (LDH-Ag 2 O/Ag) was reported by Chen et al. As shown in Figure 11c, under visible light irradiation, TC did not self-degrade, and pristine LDH showed a low degradation. After the decoration with silver nanoparticles, the photocatalytic performance increased to 65-92% in 90 min. The amount of silver used in the synthesis of the materials played an important role in their performance. It increased with the increasing content of Ag species. A higher amount of Ag species (15%) favors the recombination of e-h + , decreasing the performance of the catalyst. A stability test for the best catalyst after five cycles was performed in this case too, which showed a slight decrease in performance. These results proved good stability and high photocatalytic degradation of TC. Ag 2 O on the surface of LDH generates electron-hole pairs as a result of visible light irradiation. The ZnAl LDH, on the other hand, cannot be activated by visible light. Therefore, some photogenerated electrons from CB of Ag 2 O can be transferred to CB of ZnAlLDH because of the greater negative CB position. Following that, ZnAlLDH serves as a platform for the reactions to stimulate the formation of dissolved oxygen radicals, which are then converted to OH by interacting with H 2 O. The fact that the VB position of Ag 2 O is significantly higher than the redox potential of OH/H 2 O shows that the holes on the VB Ag 2 O cannot oxidize H 2 O to . OH. Therefore, h + on the VB of plasmonic silver would directly interact with TC. However, due to the SPR effect of silver species, additional visible light photons may be absorbed, which would result in a transfer of photoinduced electrons between the silver species. Thus, as one of the active species ( . OH, h+, and . O2), . OH significantly impacted the effective degradation of TC into intermediates and ultimately to CO 2 and H 2 O (Figure 11d) [38]. A new study demonstrated the efficiency in the photodegradation of phenol by intercalating Ag between the LDH layers and not by its traditional deposition on the LDH surface. A comparison study was performed with different species intercalated (HCO 3 − , Cl − , dodecyl sulfate, Ag(CN) 2 , and Ag) and P25. The best results were obtained on ZnAlLDH/Ag (80% degradation). In this case, after irradiation, silver nanoparticles acted as an electron source that migrated from the plasmon-excited silver to the conduction band of LDH. The superoxide radicals were created and reduced phenol due to the interaction of the e − from the conduction band with the e − acceptors [36].
Bimetallic nanoparticles supported on layered double hydroxides were also reported as good catalysts in the photodegradation of organic pollutants. A study by Darie et al. reported mono-bimetallic plasmonic (Pt/Pt-Ag) nanoparticles deposited on layered double hydroxides (ZnAlLDH and ZnFeAlLDH) as active photocatalysts in the degradation of p-nitrophenol. Their results showed that Pt-AgNPs/ZnAlLDH was more efficient compared to PtNPs/ZnAlLDH, with a 77% degradation under solar light irradiation. While introducing Fe in the LDH structure, the photocatalytic efficiency decreased drastically to 23% degradation for Pt-AgNPs/ZnFeAlLDH, even though the amount of Pt and Ag deposited on both LDHs was the same. In this case, the degradation mechanism had a different pathway. The presence of iron in the LDH structure favors the reformation of p-nitrophenol from the p-nitrophenolate ion, preventing its degradation by forbidding the electron transfer between the LDH and Pt/Pt-Ag nanoparticles. Therefore, so-called tandem photocatalysis is present. Reusing the catalyst in the three photocatalytic runs showed a slight decrease of 10% in the efficiency of the catalyst, implicitly demonstrating its stability in such processes [40]. Sahoo et al. reported the activity of bimetallic Au-Pd loaded on ZnCrLDH-MCM-41 in the synthesis of imines from oxidation and reduction of benzyl alcohol and nitrobenzene under visible light irradiation. Their results proved an increase in the photocatalytic conversion of benzyl alcohol after the deposition of bimetallic Au-Pd compared with the pristine LDH, MCM-41 or LDH-MCM-41, even compared to single metallic Au/LDH-MCM-41 and Pd/LDH-MCM-41, respectively. The same photocatalytic efficiency was obtained for the tandem reaction of imine synthesis from benzyl alcohol and nitrobenzene [112].
Regarding the applications in plasmonic catalysis of non-noble metals PNPs, Wang et al. developed an Au-Cu@LDH photocatalyst able to oxidize the benzyl alcohol and to further form an ester with methanol under visible light irradiation. In their proposed mechanism, the synergistic effect of Au-Cu alloy NPs and the surface chemistry (baseacid sits) of the Mg 3 Al-LDH support were mainly responsible for the catalytic reaction. More precisely, the Au-Cu alloy is possibly directly implicated in the cleavage of the C-H bond due to the existence of light-excited electrons that interact with the intermediate molecules. At the same time, the authors suggested that the cleavage of the O-H bond was caused by the interaction of the benzyl alcohol with the basic-acid sites of the MgAl-LDH. The unsaturated metal active sites of the alloy coordinated a benzyl alcohol intermediate due to the LSPR effect and created a metal-H bond in a metal-alcoholate-LDH system. Moreover, the light-excited electrons induced the formation of aldehydes from the metalalcoholate-LDH while also promoting the formation of O 2 •− radicals, which are further involved in the catalytic process. To conclude here, the Au-Cu plasmons showed multiple roles in this particular photocatalytic reaction [116]. Liu et al. reported a combination of light assisted thermal-driven CO 2 reduction with methane towards syngas (DRM), in the presence of a Ni/Al 2 O 3 catalyst. The suggested photomechanism is based on Au plasmonic features, which the authors extrapolated to expected Ni plasmon properties. As such, the hot electrons light-generated by NiNPs LSPR may be capable of activating the CH 4 and CO 2 molecules at a lower scale than Ag and Au but enhanced by the thermal assistance. Herein, the NiLSPR accelerated the reaction between the already activated species CH x • and O • ', and it is believed that the NiLSPR activates preponderantly the CO 2 radicals, which are further desorbed, providing more active sites for the classical thermal activation of CH 4 radicals. In this way and similar to the case of Wang et al. [116], Ni plasmon show different roles in the ambitious proposed mechanisms [117]. Recently, in a comparable synergetic system involving light and thermal input as Liu et al., Li and co-workers reported remarkable steam methane reforming (SRM) towards H 2 results. As catalyst for the photothermal experiment, the authors opted for NiNPs deposited on LDH nanosheets, Ni/NiAl-LDH. In order to prove the advantage of the photo-thermal coupling, multiple experiments were performed: (i) under only light irradiation (UV-vis) no products were detected, (ii) while in the presence of an external heat source and UV-vis light, the H 2 production reached 407.51 µmol·g −1 ·h −1 . At the same time, the catalyst exhibited UV, vis, and IR light absorption on a very broad range (between 220 and 2000 nm) owing to the SPR absorption properties of metallic NiNPs. These findings were confirmed not only by the optical characterizations performed but also with a (iii) third type of experiment, which involved the use of a Xe lamp and no external heat source. Herein, the surface temperature of the catalyst reached 671 K due to the outstanding absorption and conversion of IR light to heat energy of the Ni-containing catalysts [119]. Wang et al. focused their work on a system capable of undergoing photocatalytical water splitting reactions based upon N-doped Ti 3 C 2 (N 10 TC) MXene and NiFe-LDH. The remarkable results are attributed to the Schottky junction carrier trapping synergy created between the materials, thus a lower recombination rate, and the high capacity of the system to utilize the created plasmonic hot carriers [120].

Conclusions and Future Perspectives
This paper provides a comprehensive review on the design and fabrication of heterostructures of PNPs/LDH and their applications in the new field of hybrid plasmonic catalysis for energy related and environmental processes. As displayed by the results discussed in this review, the close conjunction and interplay of the heterostructured nano-units created plasmonic/non-plasmonic catalytic interfaces with functions that emerge from synergistically enhanced and complementary physicochemical features of the components. LDH, in their pristine form or transformed in mixed metal oxides, are endowed with advantageous features, e.g., harvesting all range of solar radiation via compositional flexibility, highly dispersed MO 6 units, and O-H surface bonds via their unique layered structure and morphology, unique memory effect property, as well as the presence of both cations and anions, which both impact the catalytic performances. Thus, LDH acts not only to confine and stabilize PNPs within the layered porous matrix but is able to establish specific metal support interactions such that the light energy harvested by the PNPs will trigger catalysis by the manifestation of plasmon-induced charge separation effect (PICS), co-catalytic effect or nano-antenna effect. However, we found that the field of plasmonic hybrid catalysis by using PNPs/LDH based heterostructures is still largely underexplored and information on PNPs/LDHs catalysts remains scarce despite that the development of high performant plasmonic heterostructures would have a strong impact on fabricating performant devices that rely on applications of plasmonic catalysis to create a sustainable society.
Several challenges remain in the development of plasmonic metal/LDH heterostructures and their application in the field of hybrid plasmonic catalysis, and we hope that these highlights will serve as a further guidance to future research.
First, controlled synthesis and design of the plasmonic metal/LDH heterostructures requires sustained research efforts in the future, focusing on both PNPs and LDH support counterparts, in terms of composition, control of particle structure and size, as well as surface/interface interactions. Obtaining high performant plasmonic nanostructures will continue to require the improvement of synthetic procedures and synthetic challenges to establish PNPs/support heteronanocomposites with high precision to tune targeted characteristics and, furthermore, to find how these characteristics are entangled to harvest the plasmonic energy in the form of electronic excitations to perform catalysis. This is a necessary prerequisite for developing performant catalysts and needs to be addressed by future research.
Next, research efforts have to focus on enhancing the LSPR response by controlling the size, shape, and surrounding environment of the PNPs. Additionally, certain limitations are yet to be overcome regarding the stability of PNPs/LDH heterostructures and the preservation of their nanomorphology during catalysis.
Furthermore, more attempts are encouraged for going beyond laboratory trials and upscaling the PNPs/LDH synthesis for their demonstration and integration in larger scale applications. Larger scale synthesis was demonstrated for the LDH materials, although compositional aspects were not completely addressed, with examples for producing large scale batches of LDHs containing transitional metals that are key photocatalytic components, or multicomponent LDH systems. This has to be followed by the PNPs synthesis and their heterostructuring with LDHs, for which only synthesis at the laboratory scale was reported until present. It was well noted that two noble plasmonic metals, i.e., Au and Ag, were dominantly used for obtaining PNPs/LDHs heterostructures, although current experimental evidence suggests that more significant results have to be established for the fast-growing field of non-noble PNPs/LDH heterostructured catalysts. Taking into account the reduced prices and the straightforward recyclability characteristics of the non-noble metals, it is important to focus on the design of catalysts with higher loadings of active metals (MeNPs) without a great cost increase. At the same time, instead of higher loadings, the non-noble metallic plasmons may be used in tandem systems (bi-metallic or alloys) with noble metal plasmons in order to create a synergistic effect. In this way, the photoactivity is considerable increased while a reduced amount of noble metals is used. Moreover, the spectral range activity of MeNPs may be extended to the near infrared (NIR) region, assuring an extra 50% of the solar light usability.
It Is further significant to develop PNPs/LDH heterostructure with strong plasmon resonance bands of LSPR by modulating the electron transfer between the nanounits. To move the field forward, we need to understand how the LDH multifunctionality can be used to increase the upper limits of the energetic charge carrier extraction from PNPs/LDH systems and how this energy is distributed within the heterostructured catalyst. Next, an important perspective would be to study and better understand the mechanism behind the photocatalysis involving PNPs/LDH.
It is anticipated that more significant results will happen in this fast growing field of plasmonic heterostructured catalysts involving the heterostructuring of PNPs with LDH. We hope that this work should serve as a motivation to achieve cutting-edge scientific results in the spectral and functional versatility of PNPs/LDH toward developing highly performant hybrid plasmonic devices for applications in catalysis.