Au nanobipyramids with Pt decoration enveloped in TiO2 nanoboxes for photocatalytic reactions

Noble metal nanocrystals and core–shell nanocomposites have attracted particular interest due to their unique optical properties originating from surface plasmon resonance (SPR) and wide applications related to the SPR effect. In this work, we designed and fabricated a new Au–Pt@TiO2 nanocomposite, in which Au nanobipyramids (AuNBPs) decorated with platinum (Pt) clusters were enveloped in mesoporous TiO2 nanoboxes with nanocavities. AuNBPs provide strong SPR absorption and localized field enhancement restricted to the cavities of TiO2 nanoboxes. The Pt nanoclusters decorated on the surface of AuNBPs can effectively modulate the charge movement and energy transfer in the photocatalytic process. The enhanced electric field provides a local thermal effect for the photocatalytic reaction and promotes the injection process of hot electrons which facilitates carrier separation. The nanoboxes with nanocavities can effectively manage the usage of localized energy and provide space for reaction. Under the cooperative effects, the photocatalytic performance was remarkably improved along with durability and stability. For the AuNBP–Pt@TiO2 nanoboxes, the rhodamine-B degradation efficiency was ∼6.5 times that of AuNBP@TiO2 nanoboxes. The mechanism of the photocatalysis process was proposed based on experimental results and simulations. Benefiting from the excellent structure and properties, the obtained nanostructure is a promising candidate in the fields of pollutant degradation and chemical reaction catalysis.


Introduction
Photocatalysis is a catalytic reaction that directly converts solar energy into chemical energy. In photocatalysis technology, it is important to design and fabricate a stable structure with recyclability and high energy utilization. Up to now, researchers have studied the synthesis and catalytic performance of a variety of substances and structures. [1][2][3][4] Usually, much attention is paid to the photoelectric efficiency and catalytic performance of metal oxide photocatalysts. 5,6 Most experiments were carried out in an open environment, which inevitably led to a loss of large amounts of energy. Therefore, it is worth studying how to effectively manage the light energy in photocatalytic reactions. On account of the unique surface plasmon resonance (SPR) effect and the tunable resonance absorption of incident light in a wide spectral region, noble metal nanostructures can effectively solve the above problems. 7,8 The highly localized electric eld and the hot electron effect of noble metal nanostructures play effective roles in promoting charge separation in photocatalytic reactions. According to previous reports, [9][10][11][12] in met-al@semiconductor nanocomposites, the SPR effect of metal nanostructures can improve the plasmon-induced resonance energy transfer (PIRET) 13,14 and hot electron injection (HEI), [15][16][17] which enhance the light utilization range and energy conversion. Particularly, for wide-gap semiconductors with excellent photocatalytic properties and little absorption of visible and near-infrared (vis-NIR) light, extending the light utilization range to vis-NIR light was a signicant aspect in photocatalyst design. 18,19 The PIRET relies on the spectral overlap between semiconductors and noble metal nanostructures. 20 In contrast, the HEI process can transfer high-energy hot electrons from metal nanostructures to the conduction band of adjacent semiconductors without spectral overlap with the semiconductors. 16 Thus, the HEI effect was considered as an excellent strategy to design photocatalysts with catalytic activity under vis-NIR light. For the HEI process, resonant plasmons localized to metal nanostructures are attenuated in a nonradiative attenuation process via interband excitation and converted to electron-hole pairs with energy higher than the metal's Fermi energy. 21 Then, the hot electrons are injected into the adjacent semiconductor conduction band, leading to an increase of the carrier concentration and electron migration rate. 7,22 As a result, the catalytic reaction would be greatly promoted. The HEI process has been extensively studied in improving photocatalysis in recent years. 23 For example, Au/ TiO 2 nanocomposites have been applied in hydrogen production from water, 24,25 photooxidation of organic molecules, 24 and the CO 2 reduction reaction 26,27 by the HEI process. Among the nanostructures with an intense SPR effect, gold nanorods (AuNRs) have been widely studied in the past two decades for their unique optical properties and potential applications. 28,29 Compared with Au nanorods, Au nanobipyramids (AuNBPs) show greater local electric eld enhancement, larger optical cross-section, narrower line widths, and better size uniformity. 30 AuNBPs were synthesized later than AuNRs, and publication of related reports began in 2007. 31 Then in 2015, an AuNBP purication strategy proposed that the purity of AuNBPs can reach close to 100%. 32 Subsequent publications were focused on the fabrication of complex nanostructures and their application based on the as-obtained AuNBPs. [33][34][35] More recently, Kan et al. 36 achieved strong SERS signal enhancement by coating an alloy shell of Au and Ag on AuNBPs. AuNBPembedded silver-platinum hollow nanostructures 37 were fabricated to monitor stepwise reduction and oxidation reactions. Their excellent electric eld enhancement effect strongly promotes the generation of hot electrons and holes. The large extinction cross-section can enhance the photocatalytic performance over a wide controllable spectral range through plasmonic sensitization. The design of AuNBP-based nanocomposites has led to the optimization of the photocatalytic activity. 38 Wang et al. 35 combined good SERS performance with catalytic activity by embedding AuNBPs into a nanoframe composed of a catalytic metal. In the AuNBP/ semiconductor composite system, charge carriers' separation is largely promoted by the strong electric eld enhancement of AuNBPs. For instance, the AuNBP@Cu 2 O nanostructure fabricated by Yang et al. 39 shows 20 times enhanced photocatalytic efficiency in the degradation of methyl orange under visible light compared to pure Cu 2 O nanoparticles. Irina Levchuk et al. 40 enhanced photocatalytic activity through insertion of AuNBPs into porous TiO 2 /SiO 2 hybrid composite lms. It is reported that TiO 2 -coated AuNBPs can be used for blocking autophagy ux and sensitizing cancer cells to proteasome inhibitor-induced death. 41 In addition to the direct use of AuNBPs, modifying with co-catalysts is an efficient approach to upgrade photocatalytic activity. Wang et al. 42 achieved several times enhanced photocatalytic activity in hydrogen production, which was attained by surface modication with Pt nanoparticles in Au-TiO 2 nanodumbbells. Consequently, reasonable design of AuNBP-based photocatalysts is critical for their excellent properties in photocatalytic reactions. 43 In this work, we designed and fabricated a new AuNBP-Pt@TiO 2 nanostructure, in which AuNBPs decorated with Pt clusters were enveloped in mesoporous TiO 2 nanoboxes with nanocavities. By subsequent growth of a Ag shell and a mesoporous TiO 2 outer shell on the surface of AuNBPs, the cavities were constructed aer removal of the Ag shell, which provides a superior reaction space for the photocatalytic reaction and promotes better separation of carriers. Simultaneously, Pt nanoclusters increase the photocatalytic efficiency of the organic degradation reaction. Finite-difference-time-domain simulation was performed to verify the enhancement and electric eld distribution of the nanostructures. The active synergy between the semiconductor nanoboxes and AuNBPs expands the respective applications of the components and provides an effective strategy for the establishment of the photocatalysis process.

Synthesis of AuNBPs
As reported previously, 8,31,32,36 a seed-mediated method was used to fabricate AuNBPs. A fresh ice-cold NaBH 4 solution (0.15 mL, 0.01 M) was injected quickly into a 10 mL aqueous solution of HAuCl 4 (0.125 mL, 0.01 M) and TSC (0.25 mL, 0.01 M). The resultant seed solution was kept at 85 C for 1.5 h to promote the formation of ve-fold twined Au seeds. The growth solution was made by sequential addition of HAuCl 4 (0.05 M, 1 mL), AgNO 3 (0.02 M, 0.5 mL), HCl (1 M, 2 mL), and AA (0.1 M, 0.8 mL) to the CTAB solution (0.1 M, 100 mL), and then shaking gently until the solution becomes colorless. Then the as-prepared seed solution (0.26 mL) was injected into the growth solution under gentle stirring for 10 s. The reaction solution was kept overnight at room temperature for the growth of AuNBPs. Typically, AuNBPs in high yield are achieved by two steps, namely Ag overgrowth based on the as-grown AuNBPs and the undisturbed storage and re-etching with NH 3 $H 2 O (8 mL) and H 2 O 2 (6%, 5 mL) solution.

Synthesis of AuNBP@TiO 2 nanoboxes
The AuNBP@TiO 2 nanoboxes were prepared in three steps. First, Au@AgNRs were prepared by a chemical reduction method. 35,43 The AuNBPs were redispersed in a CTAC solution (10 mL, 0.08 M), followed by the subsequent addition and mixing of AgNO 3 (150 mL, 0.02 M) and AA (150 mL, 0.1 M) and then stirred for 4.5 h to grow Ag shells on the AuNBPs in the form of nanorods (Au@AgNRs). The Au@AgNRs were washed with deionized water and redispersed in an SDS solution (20 mL, 0.1 M). The cationic surfactant-encapsulated Au@AgNRs were exchanged with the SDS anionic surfactant. Aer 30 min and the removal of excessive SDS, the Au@AgNRs were redispersed in 1 mL of deionized water for further mesoporous TiO 2 shell coating. For the surface TiO 2 coating, 50 mL of 15-20% TiCl 3 solution was diluted with 4 mL of water followed by dropwise injection of NaHCO 3 solution (750 mL, 0.6 M). Then the as-prepared Au@AgNR colloid was added to the system. (In the synthesis of pure amorphous TiO 2 , the as-prepared Au@AgNR colloid was replaced by SDS (0.2 mL, 0.1 M), followed by gentle stirring for 2 h.) The dispersion was kept under gentle stirring for TiO 2 coating on the surface of Au@AgNRs. The products aer reaction for 30 min (Au@AgNR@TiO 2 ) were collected by centrifugation and washed with ethanol and water (65 C) for removing the residual chemicals. The products were redispersed in 20 mL of deionized water. For the AuNBP@TiO 2 nanobox formation, the Ag shells on the AuNBP surface were removed by adding 200 mL of HNO 3 (0.1 M) and 100 mL of Fe(NO 3 ) 3 (0.02 M). The mixture was stirred for 1 h. Through this process, nanoboxes with cavities between the AuNBP cores and TiO 2 mesoporous shells were formed. The sample was washed with ethanol and stored in 20 mL of water for further use.

Synthesis of AuNBP-Pt@TiO 2 nanoboxes
AuNBP-Pt@TiO 2 nanoboxes were prepared by a chemical reduction method. 42 20 mL of the as-prepared AuNBP@TiO 2 nanoboxes was mixed with 200 mL of 0.1 M AA aer adding 30 mL of 1 mM aqueous H 2 PtCl 6 solution. The mixture was maintained at 65 C for 8 h for the formation of Pt clusters (Pt clusters were more easy to grow on the surface of AuNBPs). Then the sample was centrifuged and re-dispersed in deionized water.

Photocatalytic measurements
Photocatalytic organic degradation tests were performed in a 50 mL quartz reactor. 1 mL of the as-synthesized samples was diluted to 20 mL with an aqueous solution making the nal concentration of RhB 0.3 mM (0.25 mM SA) and sonicated for 10 min. A Xe-lamp (CEL-HXF300) was employed as the irradiation source with light ltered using a GG-420 lter(>420 nm). Magnetic stirring was applied to keep the photocatalyst particles suspended in the solution throughout the experiment. Organic degradation was measured periodically with a UV-vis spectrometer. 400 mL of reaction mixture was collected per 10 min and centrifuged at 10 000 rpm for 10 min to remove the solid catalyst. Further, a cycling stability experiment was performed under the same conditions.

Finite-difference-time-domain simulation
FDTD simulations were performed using FDTD Solutions 8.7 (Lumerical Solutions) to simulate the bare AuNBPs, AuNBP@TiO 2 core-shell structures, and AuNBP@TiO 2 nanoboxes. During the simulations, an electromagnetic pulse in the spectral range from 200 nm to 1100 nm was launched into a box containing a target nanostructure. The refractive index of the surrounding medium was 1.33, the same as that of water. The dielectric function of Au was obtained by tting the measured data of Johnson and Christy, 44 and Pt was tted from Palik's data. 45 The sizes of the AuNBPs and the AuNBP-based nanostructures were set according to the average waist widths and lengths measured from the TEM images. The refractive index of the amorphous TiO 2 shell was set as 1.65. 46 The boundary with different nanostructures inside was divided into meshes of 1 nm size.

Results and discussion
The graphic illustration of the synthesis process of AuNBP-Pt@TiO 2 nanoboxes is shown in Fig. 1a. The formation process of the TiO 2 shell and the role played by SDS are illustrated in detail in Fig. 1b. SDS micelles segregate to the Au@AgNR surface. The hydrophilic end of SDS is negatively charged in water, which would attract the titanium tri-positive ions (Ti 3+ ). As the pH reaches the hydrolysis limit of Ti 3+ , oxygen oxidized Ti 3+ to TiO 2 which was deposited on the surface of Au@AgNRs to form an outer shell. 47 Since the solubility of SDS increases sharply, aer centrifugal washing with 65 C deionized water, the SDS molecules were dissolved from the shell and removed by the water, leading to the formation of a mesoporous TiO 2 shell.
The optical spectra of nanostructures sampled in the preparation process are shown in Fig. 1c and d. The AuNBP@TiO 2 nanoboxes present a strong absorption band at about 803 nm and a weaker peak at about 505 nm (Fig. 1d), which are ascribed to the longitudinal SPR (SPR L ) and transverse SPR (SPR T ) of AuNBPs, 48 respectively. Due to the formation of TiO 2 nanoboxes, the refractive index around AuNBPs was changed. Different from the core-shell nanostructure, only the transverse part of AuNBPs was in direct contact with the TiO 2 nanoboxes. Because of the higher polarizability of the AuNBPs at the SPR L than at the transverse one, the SPR L peak has higher sensitivity. Therefore, the SPR L red shis from 738 nm to 803 nm with a full width at half maximum (FWHM) of $70 nm. The strong absorption of wavelength below 400 nm was produced by the typical bandgap transition of TiO 2 ($3.2 eV). Aer the modication with Pt clusters, the peak of SPR L red shied to $860 nm with a broad FWHM of $210 nm. The changes of absorption spectra were mainly caused by the random growth of Pt clusters on the surface of AuNBPs. Corresponding to the graphic illustration and the TEM images, FDTD solutions were applied to simulate the optical spectra of AuNBPs, AuNBP@TiO 2 nanoboxes and AuNBP-Pt@TiO 2 nanoboxes, which are shown in Fig. 1e. The FDTD method is regarded as a powerful and exible technique for studying the optical properties of metal nanostructures. 36 The plasmon absorption peaks of the AuNBPs, AuNBP@TiO 2 nanoboxes and AuNBP-Pt@TiO 2 nanoboxes were calculated to be at $741 nm, $806 nm, and $862 nm, respectively, which were in accordance with previous data obtained from experimental measurements. The results indicated that the following FDTD electric eld simulations results were reliable.
The designed morphologies were conrmed using TEM images (see Fig. 2a-f). AuNBPs were 100 nm AE 2 nm in length  Nanoscale Advances and 34 nm in diameter. Aer being coated with Ag nanoshells in the form of nanorods, the diameter of AuNBPs shows no obvious increase, and the two sharp ends of AuNBPs become round. It can be seen from Fig. 2c that the thickness of the TiO 2 shell is $30 nm. Owing to the mesoporous shell of the structure, Ag could be easily removed from the inside of the TiO 2 shell, which led to the formation of nanoboxes with cavities ( Fig. 2d and e). Aer the removal of SDS and the Ag shell, AuNBPs were mainly located in the middle of the TiO 2 nanoboxes which indicated the direct connection between the middle of AuNBPs and the TiO 2 nanoboxes. The morphology of the mesoporous TiO 2 nanoboxes showed no obvious changes aer the removal of the Ag layer by Fe 3+ , which specied the structural stability of the mesoporous shell. By comparing the element distribution of AuNBP@TiO 2 nanoboxes and AuNBP-Pt@TiO 2 nanoboxes through the element distribution mapping (Fig. 2g and h) obtained from energy dispersive spectroscopy, it can be seen that most Pt clusters are grown on the surface of AuNBPs, which conrms the porous model of the TiO 2 shell. Usually, XRD is applied to characterize the crystalline phases of prepared materials. The XRD results for the AuNBP@TiO 2 nanoboxes and the prepared amorphous TiO 2 powder are shown in Fig. 3a and b. Because the porous TiO 2 was prepared at room temperature without a further high temperature annealing process, the characteristic peaks of common crystalline TiO 2 were absent. And there is only a broad band around 21.5 , which is attributed to the amorphous form of TiO 2 (Fig. 3b) Fig. 4a. Owing to poor carrier separation of pure AuNBPs, it was difficult for highenergy electrons to participate in the photocatalytic process, which resulted in poor photocatalytic activity. AuNBPs and amorphous TiO 2 (AuNBPs + TiO 2 (Am)) mixtures show weak photocatalytic ability. The erratic contact between AuNBPs and TiO 2 (Am), and the CTAB used as a dispersant on the surface of AuNBPs affect the photocatalytic efficiency and recycling application. Comparing the AuNBP@TiO 2 core-shell structures with the designed AuNBP@TiO 2 nanoboxes, the nanoboxes show superior catalytic activity. Both of them were easy to uniformly disperse in water and to collect by centrifugation. The photocatalytic efficiency of the Pt-modied nanoboxes was also evaluated by the degradation of RhB (Fig. 4b). Commercial photocatalyst P25 was selected as the reference. To obtain samples with the same absorption of light, the spectra of P25 and the prepared nanobox photocatalyst were integrated in the vis-NIR region (400-1100 nm) followed by calculating the ratio between them. The samples were diluted with deionized water according to the calculation result. The particle number and mass of synthesized nanoboxes are much smaller than those of P25 at the same light absorption level because of the stronger vis-NIR light absorption of nanoboxes. Compared with other nanostructures mentioned before, the Pt-modied nanoboxes show the most excellent photocatalytic performance which was enhanced $6.5 times more than that of AuNBP@TiO 2 nanoboxes, and $7.3 times more than that of P25 (Fig. 4c). A degradation experiment of SA was also carried out. The degradation rates of photocatalysts are shown in Fig. 4d and e. The degradation rate of P25 reduced obviously, and the reaction rate of AuNBP@TiO 2 nanoboxes showed little change because of the different degradation process. The main difference between RhB and SA degradation is that RhB absorbs light in the vis-NIR region. Under light irradiation, electrons were excited from RhB molecules into the conduction band of TiO 2 . P25 shows photocatalytic degradation ability, even if its absorption of vis-NIR  light is weak. In order to eliminate this effect, SA with no absorption in the vis-NIR light region was selected. It can be seen from the results that the catalytic efficiency of AuNBP-Pt@TiO 2 was also affected in the case of SA. It was previously measured that amorphous TiO 2 showed little degradation of RhB, so the additional degradation of RhB was caused by the Pt cluster modication on the surface of AuNBPs. The cycling tests of AuNBP-Pt@TiO 2 nanoboxes (Fig. 4f) show durable activity in the photocatalysis reaction, which veried the recyclability and stability of the synthesized photocatalysts.  To understand the enhanced electric eld caused by the SPR excitation, three-dimensional FDTD simulation was performed to calculate the spatial distributions of the electric eld enhancement of the AuNBPs, AuNBP@TiO 2 core-shell structure and AuNBP@TiO 2 nanoboxes. As shown in Fig. 5a, the two ends of AuNBPs exhibit strong plasmon-induced electric elds caused by SPR L , with the enhancement of SPR T as shown in Fig. 5b. Aer being coated with the TiO 2 (Am) shell, the nanostructure without cavities shows stronger scattering and a lower electric eld than that with cavities (Fig. 5c). Fig. 5d and f conrm the enhanced electric eld at the interface between AuNBPs and TiO 2 . Such nano-cavities have an enhancement effect on SPR L and SPR T , thereby promoting the photocatalytic reaction. The Pt-modication of the nanoboxes caused a signicant improvement in the photocatalytic activity, which is shown in Fig. 5g and h. Aer the modication, the enhanced electric eld was redistributed because of the Pt clusters on AuNBPs. The longitudinal partial magnication suggested that the enhanced electric eld near the Pt clusters was stronger than that on the AuNBP surface ( Fig. 5i and j). Such an enhanced electric eld greatly promotes the HEI process and raises the local temperature for the further reaction.
The AuNBP-Pt@TiO 2 nanobox design was sketched to describe the effective injection process of the hot electrons (Fig. 6a). AuNBPs provide strong light absorption for the photocatalytic reaction. Excited by vis-NIR light of a specic wavelength, an enhanced electric eld is generated by SPR T . The plasmon resonance decays into electron-hole pairs. Upon crossing the Schottky barrier, electrons were injected into the TiO 2 nanoboxes. 49 Due to the bending of the energy band of TiO 2 in contact with the noble metal, 50 electrons will be transported away from the contact parts of the AuNBPs and TiO 2 nanoboxes aer injection because of the Schottky barrier, promoting the rapid separation of carriers. 51 The HEI process prompted the loss of electrons and made AuNBPs positively charged which was more suitable for the oxidation reaction. Most of the electrons that were transported to TiO 2 nanoboxes reduced Ti(IV) to Ti(III), 52 and some were injected into Pt clusters (located at TiO 2 nanoboxes) 42 which were quickly consumed by oxygen and oxidizing free-radicals. Besides rapidly absorbing electrons, the TiO 2 nanoboxes with cavities can enhance the local electric eld, which was proved by FDTD simulation. Due to the structural disorder, amorphous TiO 2 has local electronic states in the band gap, and the optical transition of carriers between these states causes a strong increase in light absorption. 53 Different from the AuNBP@TiO 2 core-shell structure, the structure with partial contact facilitates the separation of charges. The cavities offered space to separate the oxidation reaction and reduction reaction. The prolonged life of photogenerated carriers promoted the progress of the photocatalytic reaction. The strong electric eld from SPR L increases the local temperature inside the cavities. The nanobox structure reduces the dissipation of energy. 54 In addition, it also puts the organic molecules in a high-energy state, which increased the reaction activity of oxidation. As an excellent catalytic metal, Pt clusters on the surface of AuNBPs were higher performance active sites. A large number of dispersed Pt clusters expand the specic surface area of the photocatalytic reaction. In the metal-TiO 2 system, positively charged noble metal atoms are more likely to attract oxygen atoms, which activates the oxygen atoms and catalyzes the oxidation reaction. 55 A higher work function of Pt (5.65 eV) than that of Au (5.1 eV) indicates that electrons will ow from Au to Pt spontaneously, resulting in a contact potential between Pt and Au. 56,57 In addition, the loss of electrons caused by the HEI process and the stimulation of SPR L aggravated the positive charge accumulation of Au atoms. In these Au atoms, d-electron orbitals are signicantly increased, contributing to a higher density of states near the Fermi level. Attributable to the redistributed and enhanced electric eld, some of the Au atoms are highly oxidized by oxygen to generate Au-O bonds. The Au-O bonds in a state of high chemical energy not only participate in the oxidation reaction, but also activate the oxygen molecules to strengthen the photocatalytic activity. 55 Because of the long-term existence of this high-energy state, Au atoms are less likely to be poisoned by the absorption of carbonate radicals, which ensures the stability of the catalytic activity of the catalyst. On the other hand, the Pt clusters with increased electron density act as additional reduction sites, which can rapidly consume electrons to promote the carrier ow. 58 Such Pt clusters compensate to a certain extent for the lack of electron-consuming ability of amorphous TiO 2 , and also provide the possibility for AuNBP-Pt@TiO 2 nanoboxes to participate in reduction reactions such as carbon dioxide reduction and hydrogen production. 59 As shown in Fig. 6b, AuNBP-Pt@TiO 2 behaves as a miniature solar electrolytic cell reaction system. AuNBPs can be regarded as batteries that supply solar energy absorption for driving the directional ow of electrons in the system. The reaction environment constructed by the TiO 2 nanoboxes reduces the energy loss of reaction which provides high local temperature and enhanced electric eld. The positive synergy of the catalyst and the cocatalyst strategically adjusted the energy transfer in the photocatalytic reaction, and signicantly improved the light utilization rate and photocatalytic activity.

Conclusion
In summary, in order to modulate the energy transfer in the photocatalytic process, we designed and fabricated a new Au-Pt@TiO 2 nanostructure, in which AuNBPs decorated with Pt clusters were enveloped in TiO 2 nanoboxes. The photocatalytic performance of the obtained nanostructure was remarkably improved in the degradation of RhB and SA. Based on the experimental and simulated results, the photocatalytic reaction of the photovoltaic-electrolysis model was proposed. In this nanocomposite, AuNBPs exhibit strong SPR absorption in the vis-NIR region. The HEI effect and enhanced electric eld localized in the nanocavities of TiO 2 nanoboxes promote charge separation and the hot electron injection process. The nanobox structure can effectively manage the usage of localized energy. Pt nanoclusters on the surface of AuNBPs were located in an enhanced eld and promoted to a higher-level state that was appropriate for accepting and consuming electrons. Under the cooperative effects of plasmonic Au metal, catalytic Pt nanoclusters and TiO 2 nanocavities, the photocatalytic performance of the obtained nanostructure was remarkably improved in the degradation of RhB and SA. This nanostructure not only realizes the stability of the structure, but also provides a new strategy for making full use of cooperative effects in photocatalytic performance, which offers better means for using solar energy to carry out environmental governance and develop clean energy. It also offers design of articial photosynthesis systems with promising application prospects.

Conflicts of interest
The authors declare no conicts of interest.