Controlled Synthesis of Au Nanocrystals-Metal Selenide Hybrid Nanostructures toward Plasmon-Enhanced Photoelectrochemical Energy Conversion

A simple method for the controllable synthesis of Au nanocrystals–metal selenide hybrid nanostructures via amino acid guiding strategy is proposed. The results show that the symmetric overgrowth mode of PbSe shells on Au nanorods can be precisely manipulated by only adjusting the initial concentration of Pb2+. The shape of Au–PbSe hybrids can evolve from dumbbell-like to yolk-shell. Interestingly, the plasmonic absorption enhancement could be tuned by the symmetry of these hybrid nanostructures. This provides an effective pathway for maneuvering plasmon-induced energy transfer in metal–semiconductor hybrids. In addition, the photoactivities of Au–PbSe nanorods sensitized TiO2 electrodes have been further evaluated. Owing to the synergism between effective plasmonic enhancement effect and efficient interfacial charge transfer in these hybrid nanostructures, the Au–PbSe yolk-shell nanorods exhibit an outstanding photocurrent activity. Their photocurrent density is 4.38 times larger than that of Au–PbSe dumbbell-like nanorods under light irradiation at λ > 600 nm. As a versatile method, the proposed strategy can also be employed to synthesize other metal–selenide hybrid nanostructures (such as Au–CdSe, Au–Bi2Se3 and Au–CuSe).


Synthesis of Au-PbSe Hybrid NRs
In a typical procedure, Gly [Pb 2+ ] that acted as the Pb 2+ precursor was prepared by 0.02 mL of 0.1 M Pb(C 2 H 3 O 2 ) 2 ·3H 2 O and 1.0 mL of 0.2 M Gly in a 10 mL round-bottom test tube, followed by the addition of 1 mL of the as-prepared Au@Se NRs seed. The pH of the reaction solution was regulated to 9.8 by injecting 2 M NaOH solution. Subsequently, 0.02 mL of 0.1 M AA was added and kept at 80 • C under vigorously stirring for 90 min. The obtained products were centrifuged at 8000 rpm for 9 min, and then redispersed in water solution. The obtained sample was Au-PbSe yolk-shell hybrid NRs.

NWs Film Electrodes
Firstly, TiO 2 nanowires (NWs) film was grown on fluorine-doped tin oxide (FTO) glass substrate by the hydrothermal method. 7.5 mL of HCl was diluted with 7.5 mL ultrapure water and mixed with 0.25 mL C 16 H 36 O 4 Ti in a 50 mL beaker. After stirring for 30 min, this white suspension mixture and a clean FTO glass substrate were transferred to a 25 mL Teflon-lined stainless-steel autoclave, where the FTO substrate was tilted 45 degrees in the solution. The sealed autoclave was heated in an electric oven at 150 • C for 5 h, and then let it cool down to room temperature slowly. A white TiO 2 NWs film was uniformly deposited on the FTO glass substrate, which was thoroughly washed with ultrapure water and then dried at 60 • C in a vacuum. The sample was annealed in air at 550 • C for 3 h to improve the crystallinity of TiO 2 NWs. Subsequently, to obtain TiO 2 NWs electrodes sensitized with Au-PbSe yolk-shell hybrid NRs, the adsorbent was prepared by adding 10 mg of Au-PbSe NRs into 1 mL of 0.17 M alcohol solution. The obtained TiO 2 NWs film was immersed into it for 3 min, then was thoroughly washed with ethanol and dried at 50 • C in a vacuum. After repeated the adsorption process three times, the expected (Au-PbSe yolk-shell NRs)@TiO 2 NWs film electrode was obtained. (PbSe NCs)@TiO 2 and (Au-PbSe dumbbell NRs)@TiO 2 NWs electrodes were obtained by the same way, excepting using the equal amounts of counterparts instead of Au-PbSe yolk-shell NRs in the adsorption process.

Photocurrent Response and Incident Photon to Current Conversion Efficiency (IPCE) Measurements
TiO 2 NWs film was fabricated into photoanodes by soldering a copper wire onto a bare part of the FTO substrate. The working electrode area is 1 cm 2 . Na 2 SO 3 (0.25 M) and Na 2 S (0.35 M) aqueous solution (pH ≈ 12), Ag/AgCl, and Pt were employed as electrolyte, reference electrode, and counter electrode, respectively. Photocurrent experiments were carried out at a scan rate of 10 mV/s under the solar simulator (Beijing SOFN photoelectric instruments Co. Ltd., 7IS0503A, Beijing, China) using a 350 W xenon lamp equipped with an air mass 1.5 global (AM 1.5G) filter as illumination source (100 mW/cm 2 ). After adding a 600 nm long-pass filter to AM 1.5G simulated sunlight, the light irradiation power change to 3.8 mW/cm 2 . The IPCE spectra were measured by using a 150 W Xenon lamp equipped with a monochromator.

Controllable Synthesis of Au-PbSe Hybrid NRs
In this work, Au NRs are chosen as our initial materials because of their fascinating optical properties. A schematic outline of the amino acid guidance strategy is shown in Figure 1. The preparation progress can be divided into two steps. Firstly, an amorphous Se shell is deposited on the Au NRs by reducing SeO 2 with AA. When CTAB is used as the stabilizer and morphology inducer, the end-opened Au@Se core@shell NRs can be obtained owing to the anisotropy of NR and the strong affinity between Au and Se. In order to further obtain metal selenide nanoshells, Au@Se NRs are used as seeds and Se sources in the next step. Previous literatures have revealed that amino acids can interact with metal clusters through the amine and carboxylic groups [53], Gly molecules can selectively adsorb on two ends of Au@Se NRs by the anchoring bonds. In addition, Gly can be also combined with metal ions to form a complex. Therefore, Gly can act as a transporter in the reaction, carrying metal ions from the solution to the end regions of Au NRs. Subsequently, Se atoms in the shells turned into Se 2− and Se 4+ ions by disproportionation reaction. The solution is adjusted to an appropriate pH value with NaOH aqueous solution, when Se 2− and metal ions encounter in the solution, metal selenide nanocrystals are expected to form and further facilitate the disproportionation process of Se. In addition, Se 4+ ions will be reduced back to Se 0 again through AA in the solution and continue to participate in the above reaction. As such, the Au-selenide hybrid NRs with hollow shells are obtained. Furthermore, the symmetry manipulating of semiconductor hollow shells can be realized by changing the initial concentration of the added cation precursors. The major reactions involved in this process can be summarized as the following [54,55]: Taking Au-PbSe hybrid NRs as an example, the morphology and structure characterizations at each growth stage are characterized in detail by TEM images in Figure 2a-c. The initial Au NRs synthesized by a seed-mediated growth method exhibit regular rod shape, the corresponding average length and width are about 56 and 16 nm, respectively. After the addition of SeO2 and AA, incubating at 38 °C for 5 h, the designed Au@Se core@shell NRs seeds are shown in Figure 2b. As we can see, when the added amount of Se source is 20 L of 0.1 M, the average thickness of Se shell is about 22 nm. Subsequently, as 20 L of 0.1 M Pb 2+ precursor is added, the closed Au-PbSe hybrid NRs with transversely symmetrical hollow shells are achieved. The corresponding TEM images shown in Figure 2c reveal that Au NRs are embedded on the longitudinal axis of hollow ellipsoidal shells. There is a 12 nm gap between the Au core and the external PbSe and the semiconductor nanoshells of about 13.8 nm shells are wrapped around the NRs, which is a typical yolk-shell nanostructure. Interestingly, the Au NRs yolk keeps close contacts with the semiconductor shells at both ends, which provides an easy access for the interfacial electron interactions. In order to obtain more crystallographic details, XRD analyses were performed for the samples at different reaction stages. As shown in Figure 2d, the diffraction peaks from Au can be well identified according to joint committee on powder diffraction standards (JCPDS) cards no. 04-0784. The result indicates that the crystalline phase of the initial Au NRs is cubic. After coating Se shells on the sides of Au cores, no new diffraction peaks are found from the samples, indicating that the Se shells are amorphous. As for Au-PbSe hybrid NRs, a new XRD pattern emerges, which can be indexed as the cubic PbSe phase (JCPDS card no. 06-0354). Figure 2e is HRTEM image of the individual hybrid NR at the interface of Au NR yolk and PbSe shell. As expected, a lattice plane spacing of 0.306 nm in the shell region is observed, which agrees well with the (200) lattice planes of the cubic PbSe crystal. Also, the lattice plane distance of 0.235 nm in the yolk region corresponds to the (111) planes of face-centered cubic (fcc) Au. To further confirm the composition of the samples, the corresponding EDS is exhibited in Figure 2f, the spectrum shows strong Au, Pb, and Se peaks in addition to the C, O, and Cu peaks generated by the copper grid. This result demonstrates the existences of Au, Pb, and Se elements in the yolk-shell nanostructures. Additionally, the HAADF-STEM imaging and EDS elemental mapping of single nanoparticle are displayed in Figure 2g-j. As can be seen, Pb (red) and Se (cyan) are uniformly distributed in the shell region, and the yolk is composed of Au (blue), demonstrating that the well-defined Au-PbSe yolk-shell hybrid nanostructures are obtained in our experiments. Taking Au-PbSe hybrid NRs as an example, the morphology and structure characterizations at each growth stage are characterized in detail by TEM images in Figure 2a-c. The initial Au NRs synthesized by a seed-mediated growth method exhibit regular rod shape, the corresponding average length and width are about 56 and 16 nm, respectively. After the addition of SeO 2 and AA, incubating at 38 • C for 5 h, the designed Au@Se core@shell NRs seeds are shown in Figure 2b. As we can see, when the added amount of Se source is 20 µL of 0.1 M, the average thickness of Se shell is about 22 nm. Subsequently, as 20 µL of 0.1 M Pb 2+ precursor is added, the closed Au-PbSe hybrid NRs with transversely symmetrical hollow shells are achieved. The corresponding TEM images shown in Figure 2c reveal that Au NRs are embedded on the longitudinal axis of hollow ellipsoidal shells. There is a 12 nm gap between the Au core and the external PbSe and the semiconductor nanoshells of about 13.8 nm shells are wrapped around the NRs, which is a typical yolk-shell nanostructure. Interestingly, the Au NRs yolk keeps close contacts with the semiconductor shells at both ends, which provides an easy access for the interfacial electron interactions. In order to obtain more crystallographic details, XRD analyses were performed for the samples at different reaction stages. As shown in Figure 2d, the diffraction peaks from Au can be well identified according to joint committee on powder diffraction standards (JCPDS) cards no. 04-0784. The result indicates that the crystalline phase of the initial Au NRs is cubic. After coating Se shells on the sides of Au cores, no new diffraction peaks are found from the samples, indicating that the Se shells are amorphous. As for Au-PbSe hybrid NRs, a new XRD pattern emerges, which can be indexed as the cubic PbSe phase (JCPDS card no. 06-0354). Figure 2e is HRTEM image of the individual hybrid NR at the interface of Au NR yolk and PbSe shell. As expected, a lattice plane spacing of 0.306 nm in the shell region is observed, which agrees well with the (200) lattice planes of the cubic PbSe crystal. Also, the lattice plane distance of 0.235 nm in the yolk region corresponds to the (111) planes of face-centered cubic (fcc) Au. To further confirm the composition of the samples, the corresponding EDS is exhibited in Figure 2f, the spectrum shows strong Au, Pb, and Se peaks in addition to the C, O, and Cu peaks generated by the copper grid. This result demonstrates the existences of Au, Pb, and Se elements in the yolk-shell nanostructures. Additionally, the HAADF-STEM imaging and EDS elemental mapping of single nanoparticle are displayed in Figure 2g-j. As can be seen, Pb (red) and Se (cyan) are uniformly distributed in the shell region, and the yolk is composed of Au (blue), demonstrating that the well-defined Au-PbSe yolk-shell hybrid nanostructures are obtained in our experiments.

Growth Kinetics and Symmetry Controlling of Au-PbSe Hybrid NRs
We monitored the evolution of shape for the products obtained at different reaction stages with corresponding TEM images in Figure 3. Figure 3a exhibits the initial Au@Se NRs with a uniform nanoshell. It is notable that Se atoms mainly distribute in the shell region, while Pb 2+ ions disperse in the solution. The diffusion flux of Se 2− ion is obviously higher than that of Pb 2+ ion at the reaction interface. After reaction for 5 min, some small voids appear in the inner of shells owing to the Kirkendall effect [56,57]. As displayed in Figure 3b. Meanwhile, a set of distinct lattice fringes emerge on the outer layer of the shell, which indicates that the PbSe NCs with cubic phase are beginning to form. Continue to reaction for 25 min, Figure 3c shows the Kirkendall voids coalesce into a bigger one via the fast surface diffusion of Se atoms. With the reaction proceeding, the expected Au-PbSe yolk-shell hybrid nanostructure is obtained at 60 min, as shown in Figure 3d. What's more, two ends of the NRs are wrapped by PbSe NCs at the initial stage, it can be attributed to the selectively adsorption of Gly[Pb 2+ ] complexes on the ends of Au NRs. Their corresponding low magnification TEM images are displayed in Figure S1. As such, it is reasonable to assume that the structures of hybrid NRs are determined by the combined actions of Kirkendall effect and Gly guiding mechanism in our experiments.

Growth Kinetics and Symmetry Controlling of Au-PbSe Hybrid NRs
We monitored the evolution of shape for the products obtained at different reaction stages with corresponding TEM images in Figure 3. Figure 3a exhibits the initial Au@Se NRs with a uniform nanoshell. It is notable that Se atoms mainly distribute in the shell region, while Pb 2+ ions disperse in the solution. The diffusion flux of Se 2− ion is obviously higher than that of Pb 2+ ion at the reaction interface. After reaction for 5 min, some small voids appear in the inner of shells owing to the Kirkendall effect [56,57]. As displayed in Figure 3b. Meanwhile, a set of distinct lattice fringes emerge on the outer layer of the shell, which indicates that the PbSe NCs with cubic phase are beginning to form. Continue to reaction for 25 min, Figure 3c shows the Kirkendall voids coalesce into a bigger one via the fast surface diffusion of Se atoms. With the reaction proceeding, the expected Au-PbSe yolk-shell hybrid nanostructure is obtained at 60 min, as shown in Figure 3d. What's more, two ends of the NRs are wrapped by PbSe NCs at the initial stage, it can be attributed to the selectively adsorption of Gly[Pb 2+ ] complexes on the ends of Au NRs. Their corresponding low magnification TEM images are displayed in Figure S1. As such, it is reasonable to assume that the structures of hybrid NRs are determined by the combined actions of Kirkendall effect and Gly guiding mechanism in our experiments.  To further test this hypothesis, the diffusion flux of precursors at the reaction interface can be tuned by their initial concentration in this experiment. Here, there are four parallel samples with the same seed of Au@Se NRs, and the related initial molar concentrations Pb 2+ (C(Pb 2+ )) are set to 0.25 mM, 0.5 mM, 0.75 mM and 1.0 mM, respectively. Corresponding TEM images of the Au-PbSe hybrid nanostructures are exhibited in Figure 4a-d. At a low Pb 2+ ion concentration, most of Pb 2+ ions in the solution are transported to both ends of the Au@Se NRs in the forms of Gly[Pb 2+ ] complexes. Meanwhile, Se atoms in the shells are reduced to Se 2− ions by AA and diffused into the solution under the action of concentration gradient force. Once Se 2− ions encounter Pb 2+ ions at the end regions of Au NRs, PbSe NCs will be formed. When C(Pb 2+ ) = 0.25 mM, owing to the binding of Gly to metal ions, the diffusion rate of Se 2− ion is higher than that of Pb 2+ ion in the end regions of NRs, which inhibit the formation of Kirkendall voids. Hence, the Gly-guiding mechanism plays a dominant role in the growth of PbSe at this moment. As shown in Figure 4a, Au-PbSe NRs with two porous PbSe NCs on the ends of NRs are obtained, in which the semiconductor shell has a longitudinally symmetrical distribution. Here, we call them as Au-PbSe porous-dumbbell NRs. With increasing the concentration of Pb 2+ in the reaction solution, the diffusion rate of Pb 2+ ions increases. As C(Pb 2+ ) increases to 0.5 mM, the diffusion flux of Pb 2+ ions is larger than that of Se 2-ions at the reaction interface. As shown in Figure 4b, the Au-PbSe nanodumbbells with longitudinally symmetrical hollow shells are observed and called as hollow-dumbbell NRs, which implies that two mechanisms of Kirkendall effect and Gly-guiding metal cation transport exist simultaneously in the growth process. In addition, the increase of Pb 2+ diffusion rate also causes the reaction interface to move towards Se shell area. As expected, when C(Pb 2+ ) increases to 0.75 mM, umbrella-shape PbSe NC gradually forms and then curls toward the sides of NR, the corresponding TEM image is displayed in Figure 4c. Finally, under the joint action of these two mechanisms, the Au-PbSe yolk-shell nanostructure with transversely symmetric hollow shell can be obtained at C(Pb 2+ ) = 1 mM. The results are illustrated in Figure 4d. The HAADF-STEM imaging in conjunction with EDS elemental mapping in Figure 4e further reveal the coexistence of Au NRs and PbSe cap regions for hollow nanodumbbells. As thus, the symmetry of the hollow PbSe shells on Au NRs can be manipulated from longitudinally to transversely symmetric distributions by simply adjusting the Meanwhile, Se atoms in the shells are reduced to Se 2− ions by AA and diffused into the solution under the action of concentration gradient force. Once Se 2− ions encounter Pb 2+ ions at the end regions of Au NRs, PbSe NCs will be formed. When C(Pb 2+ ) = 0.25 mM, owing to the binding of Gly to metal ions, the diffusion rate of Se 2− ion is higher than that of Pb 2+ ion in the end regions of NRs, which inhibit the formation of Kirkendall voids. Hence, the Gly-guiding mechanism plays a dominant role in the growth of PbSe at this moment. As shown in Figure 4a, Au-PbSe NRs with two porous PbSe NCs on the ends of NRs are obtained, in which the semiconductor shell has a longitudinally symmetrical distribution. Here, we call them as Au-PbSe porous-dumbbell NRs. With increasing the concentration of Pb 2+ in the reaction solution, the diffusion rate of Pb 2+ ions increases. As C(Pb 2+ ) increases to 0.5 mM, the diffusion flux of Pb 2+ ions is larger than that of Se 2ions at the reaction interface. As shown in Figure 4b, the Au-PbSe nanodumbbells with longitudinally symmetrical hollow shells are observed and called as hollow-dumbbell NRs, which implies that two mechanisms of Kirkendall effect and Gly-guiding metal cation transport exist simultaneously in the growth process. In addition, the increase of Pb 2+ diffusion rate also causes the reaction interface to move towards Se shell area. As expected, when C(Pb 2+ ) increases to 0.75 mM, umbrella-shape PbSe NC gradually forms and then curls toward the sides of NR, the corresponding TEM image is displayed in Figure 4c. Finally, under the joint action of these two mechanisms, the Au-PbSe yolk-shell nanostructure with transversely symmetric hollow shell can be obtained at C(Pb 2+ ) = 1 mM. The results are illustrated in Figure 4d. The HAADF-STEM imaging in conjunction with EDS elemental mapping in Figure 4e further reveal the coexistence of Au NRs and PbSe cap regions for hollow nanodumbbells. As thus, the symmetry of the hollow PbSe shells on Au NRs can be manipulated from longitudinally to transversely symmetric distributions by simply adjusting the initial Pb 2+ concentration, which is ascribed to the combined actions of Kirkendall effect and the glycine-guiding cation transport. In addition, as exhibited in Figure S2, Au-PbSe yolk-shell hybrid NRs with different shell thicknesses and nanovoid sizes are also achieved by adjusting Se shell of Au@Se nanoseeds. initial Pb 2+ concentration, which is ascribed to the combined actions of Kirkendall effect and the glycine-guiding cation transport. In addition, as exhibited in Figure S2, Au-PbSe yolk-shell hybrid NRs with different shell thicknesses and nanovoid sizes are also achieved by adjusting Se shell of Au@Se nanoseeds. As a general method, our strategy can be extended to the synthesis of other metal-selenide hybrid nanostructures. By simply replacing the Gly[Pb 2+ ] complexes with corresponding cation precursors and regulating the pH value of the system, the Au-CdSe, Au-Bi2Se3 and Au-CuSe hybrid nanostructures can be successfully obtained. The detailed operation processes are described in the Electronic Supplementary Information. The morphology and detailed crystallographic structures of the corresponding hybrid NRs are shown in Figure S3. As we can see, all the prepared hybrid nanostructures have uniform rod-like Au cores, and Au NRs are wrapped with semiconductor nanoshells. More interestingly, two ends of Au NRs are clearly enclosed with semiconductor counterparts in three samples. The results further confirm the guiding roles of Gly in the growth of hybrid nanostructures. Furthermore, Au-PbSe yolk-shell nanocubes and triangular nanoprisms can also be achieved by the similar method, as shown in the Figure S4. Compared with the other strategies (i.e., cation exchange, overgrowth assisted with Ag wetting layer), the above growth As a general method, our strategy can be extended to the synthesis of other metal-selenide hybrid nanostructures. By simply replacing the Gly[Pb 2+ ] complexes with corresponding cation precursors and regulating the pH value of the system, the Au-CdSe, Au-Bi 2 Se 3 and Au-CuSe hybrid nanostructures can be successfully obtained. The detailed operation processes are described in the Electronic Supplementary Information. The morphology and detailed crystallographic structures of the corresponding hybrid NRs are shown in Figure S3. As we can see, all the prepared hybrid nanostructures have uniform rod-like Au cores, and Au NRs are wrapped with semiconductor nanoshells. More interestingly, two ends of Au NRs are clearly enclosed with semiconductor counterparts in three samples. The results further confirm the guiding roles of Gly in the growth of hybrid nanostructures. Furthermore, Au-PbSe yolk-shell nanocubes and triangular nanoprisms can also be achieved by the similar method, as shown in the Figure S4. Compared with the other strategies (i.e., cation exchange, overgrowth assisted with Ag wetting layer), the above growth scheme of metal-selenide hybrid nanostructures based on Se nanoshells and amino acid guiding strategy obviously possesses some advantages such as good crystallinity, controllable shell morphology and no introduction of other impurities (such as Cu 2+ or Ag + ).

Optical Properties of Au-PbSe NRs with Different Shells Distributions
It is known that the optical properties of metal-semiconductor plasmonic nanostructures are closely related to the distribution of semiconductor component. The controllable morphology of Au-PbSe hybrid NRs can be used to regulate their SPR properties. As see in Figure 5, the SPR peaks of original Au NRs are observed at 518 nm and 752 nm, respectively. After 13 nm Se shell is coated, the corresponding peaks of Au@Se NRs, respectively, shift to 578 nm and 1018 nm, accompanying with the emergence of a new transverse resonance mode at 680 nm. Those can be attributed to the high refractive index of the Se layer. Nanomaterials 2020, 10, x FOR PEER REVIEW 9 of 16 scheme of metal-selenide hybrid nanostructures based on Se nanoshells and amino acid guiding strategy obviously possesses some advantages such as good crystallinity, controllable shell morphology and no introduction of other impurities (such as Cu 2+ or Ag + ).

Optical Properties of Au-PbSe NRs with Different Shells Distributions
It is known that the optical properties of metal-semiconductor plasmonic nanostructures are closely related to the distribution of semiconductor component. The controllable morphology of Au-PbSe hybrid NRs can be used to regulate their SPR properties. As see in Figure 5, the SPR peaks of original Au NRs are observed at 518 nm and 752 nm, respectively. After 13 nm Se shell is coated, the corresponding peaks of Au@Se NRs, respectively, shift to 578 nm and 1018 nm, accompanying with the emergence of a new transverse resonance mode at 680 nm. Those can be attributed to the high refractive index of the Se layer. Subsequently, for porous (C(Pb 2+ ) = 0.25 mM) and hollow (C(Pb 2+ ) = 0.5 mM) Au-PbSe nanodumbbells, their T-SPR peaks keep almost unchanged in comparison to the original Au NRs, because semiconductor component is mainly distributed at both ends of the NRs. As C(Pb 2+ ) is adjusted from 0.5 to 0.75 mM, the hollow semiconductor components change into umbrella-shaped caps at both ends of the NRs. Their corresponding L-SPR peak exhibits a slightly blue shift and the T-SPR peak shows a red shift, owning to the formation of a new surrounding environment. Meanwhile, the hollow nanodumbbells shows a significantly enhanced absorption peak in the NIR region, which might be due to the strong longitudinal coupling between plasmons and excitons in the hybrids. When the closed hollow shells with transverse symmetry are formed (C(Pb 2+ ) = 1 mM), the L-SPR peak of Au-PbSe yolk-shell NRs redshifts to 1450 nm. Most interestingly, a significant enhancement of T-SPR band at visible region is displayed in the yolk-shell structures, it might be ascribed to the strong transverse coupling between plasmons and excitons in the hybrids. The results provide an effective pathway for maneuvering optical properties of metal-semiconductor hybrids by the distribution of hollow nanoshells. The local field confinements and enhancements of the metal-semiconductor hybrids with different symmetric hollow shells are further revealed by using FDTD simulations in Figure S5. The L-SPR and T-SPR wavelengths of the starting Au NRs are located at 780 nm and 509 nm, respectively. After the PbSe hollow shells were grown on the Au NRs, the dumbbell nanostructure exhibits corresponding T-SPR enhancement, and the core-shell structures exhibit L-SPR enhancement. Their variation tendency is in accord with the above experimental results. Three kinds of plasmonic nanostructures exhibit different field enhancement Subsequently, for porous (C(Pb 2+ ) = 0.25 mM) and hollow (C(Pb 2+ ) = 0.5 mM) Au-PbSe nanodumbbells, their T-SPR peaks keep almost unchanged in comparison to the original Au NRs, because semiconductor component is mainly distributed at both ends of the NRs. As C(Pb 2+ ) is adjusted from 0.5 to 0.75 mM, the hollow semiconductor components change into umbrella-shaped caps at both ends of the NRs. Their corresponding L-SPR peak exhibits a slightly blue shift and the T-SPR peak shows a red shift, owning to the formation of a new surrounding environment. Meanwhile, the hollow nanodumbbells shows a significantly enhanced absorption peak in the NIR region, which might be due to the strong longitudinal coupling between plasmons and excitons in the hybrids. When the closed hollow shells with transverse symmetry are formed (C(Pb 2+ ) = 1 mM), the L-SPR peak of Au-PbSe yolk-shell NRs redshifts to 1450 nm. Most interestingly, a significant enhancement of T-SPR band at visible region is displayed in the yolk-shell structures, it might be ascribed to the strong transverse coupling between plasmons and excitons in the hybrids. The results provide an effective pathway for maneuvering optical properties of metal-semiconductor hybrids by the distribution of hollow nanoshells. The local field confinements and enhancements of the metal-semiconductor hybrids with different symmetric hollow shells are further revealed by using FDTD simulations in Figure  S5. The L-SPR and T-SPR wavelengths of the starting Au NRs are located at 780 nm and 509 nm, respectively. After the PbSe hollow shells were grown on the Au NRs, the dumbbell nanostructure exhibits corresponding T-SPR enhancement, and the core-shell structures exhibit L-SPR enhancement.
Their variation tendency is in accord with the above experimental results. Three kinds of plasmonic nanostructures exhibit different field enhancement distributions, indicating that the symmetry of shells affects greatly the optical properties of the hybrid NRs. Here, the Au-PbSe yolk-shell hybrid NRs with transverse shells have a strong T-SPR band in the visible region, besides considerable longitudinal resonance absorption. As thus, the broad SPR absorption bands from Au-PbSe NRs, ranged from Vis to NIR region, match well with the peak wavelength of solar spectrum, allowing for the potential solar applications.

Photoelectrochemical Performances Tests
The photoelectrochemical tests of TiO 2 NWs photoanodes sensitized by Au-PbSe hybrid NRs with different symmetry were further performed in a three-electrode cell, with Ag/AgCl as the reference electrode and a Pt wire as the counter electrode. In comparison, TiO 2 NWs electrodes are sensitized with hollow PbSe NCs, Au-PbSe dumbbell-like and yolk-shell NRs, which are labeled as (PbSe NCs)@TiO 2 , (Au-PbSe dumbbell NRs)@TiO 2 and (Au-PbSe yolk-shell NRs)@TiO 2 , respectively. All sensitizers had the same mass of corresponding components as described in the Table S1. TEM images of the sensitizers and corresponding extinction spectra of the sensitized TiO 2 electrodes are shown in Figure S6 and S7 respectively. The typical SEM images of (Au-PbSe NRs)@TiO 2 electrode are shown in Figure S8. As shown in Figure 6a, it displays the I-t curves for four parallel electrodes under white-light (AM 1.5G, 100 mW/cm 2 ). A clear photo-switching behavior is observed, and the photocurrent of all the sensitized electrodes are enhanced compared with that of TiO 2 NWs substrate, which implies that there exists an effective photoelectron transfer channel from sensitizer to TiO 2 . The stable photocurrents of 0.49, 0.46, and 0.63 mA/cm 2 were correspondingly obtained for PbSe@TiO 2 , (Au-PbSe dumbbell NRs)@TiO 2 and (Au-PbSe yolk-shell NRs)@TiO 2 NWs electrode. The results suggest that the photocurrent response is obviously dependent on the shell symmetry for metal-semiconductor hybrid nanostructures sensitized electrode. The corresponding photocurrent density-applied potential characteristics are presented in Figure S9.
To further explore the effect of Au-PbSe NRs with different symmetrical shells on the photoactivities of their sensitized TiO 2 electrodes, Figure 6b shows the I-t curves under light irradiation at λ > 600 nm. As seen, no obvious photocurrent response is detected in the pure TiO 2 NWs substrate under the same testing conditions. After sensitized with PbSe NCs, a stable photocurrent with a density of 12.25 µA/cm 2 can be observed, which indicates that there is an effective photoelectron transfer process from the PbSe NCs to the TiO 2 NWs. More interestingly, the intensity of the photoelectric signal is decreased to 10.62 µA/cm 2 for (Au-PbSe dumbbell NRs)@TiO 2 electrode. By contrast, the photocurrent density of (Au-PbSe yolk-shell NRs)@TiO 2 is 4.38 times that.
To understand the charge-transfer process, electrochemical impedance spectroscopy (EIS) experiments were performed at open circuit potential under light illumination (λ > 600 nm). Here, R s denotes the contact resistances of the electrochemical device, CPE denotes the capacitance phase element, and R ct denotes the interfacial charge transfer resistance. As shown in Figure 6c, the values of R ct are calculated to be 13.35, 6.74, 2.88 and 1.81 KΩ for TiO 2 , (PbSe NCs)@TiO 2 , (Au-PbSe dumbbell NRs)@TiO 2 and (Au-PbSe dumbbell NRs)@TiO 2 electrodes, respectively. R ct of (PbSe NCs)@TiO 2 electrode is significantly smaller than that of pure TiO 2 electrode. This indicates that there exists a favorable energy level alignment between TiO 2 NWs and hollow PbSe NCs. Among them, (Au-PbSe yolk-shell NRs)@TiO 2 has the smallest radius in comparison to the other three electrodes. Therefore, it manifests the fastest charge carriers transfer rate. The physics behind this result can be explained by the highly efficient photoexcitation and electron-hole separation efficiency resulting from the unique spatial architecture of Au-PbSe yolk-shell nanostructures. As for dumbbell-like Au-PbSe NRs, 27.5 nm PbSe NCs are symmetrically distributed on both ends of Au NRs (see in Figure S6). Because of the quantum size effect, it will induce the changes of the energy band structures of PbSe NCs and the formation of unfavorable energy level alignment in the PbSe-TiO 2 heterojunction. As a consequence, the transfer of electrons from PbSe to TiO 2 electrode was greatly inhibited. (Au-PbSe dumbbell NRs)@TiO 2 electrode exhibits the higher interfacial charge transfer resistance than the other sensitized electrodes. These results further confirm the importance of structure and interface optimization for the photoelectric conversion of metal-semiconductor hybrid nanomaterials, which are highly consistent with the above photocurrent tests. To verify whether the observed photoactivity enhancement of (Au-PbSe yolk-shell NRs)@TiO 2 electrode comes from the plasmon excitation of the hybrid NRs, IPCE for (PbSe NCs)@TiO 2 and (Au-PbSe yolk-shell NRs)@TiO 2 electrodes were also performed. Two electrodes are subjected to an incident light with wavelength 600-1000 nm. IPCE values at specific wavelengths are calculated are shown in the Electronic Supplementary Information. As presented in Figure 6d, the measured IPCE action spectrum of the (Au-PbSe yolk-shell NRs)@TiO 2 electrode matches well with its corresponding SPR absorption spectrum. Additionally, different from (PbSe NCs)@TiO 2 , (Au-PbSe yolk-shell NRs)@TiO 2 exhibits two evident IPCE enhancement bands located at 670 and 980 nm, which suggests that Au NRs and PbSe nanoshells in the yolk-shell NRs can synergistically promote the photoelectron excitation due to the effective plasmon-exciton interaction under Vis-NIR light (λ > 600 nm) irradiation.  To understand the charge-transfer process, electrochemical impedance spectroscopy (EIS) experiments were performed at open circuit potential under light illumination ( > 600 nm). Here, Rs denotes the contact resistances of the electrochemical device, CPE denotes the capacitance phase element, and Rct denotes the interfacial charge transfer resistance. As shown in Figure 6c, the values of Rct are calculated to be 13.35, 6.74, 2.88 and 1.81 KΩ for TiO2, (PbSe NCs)@TiO2, (Au-PbSe dumbbell NRs)@TiO2 and (Au-PbSe dumbbell NRs)@TiO2 electrodes, respectively. Rct of (PbSe NCs)@TiO2 electrode is significantly smaller than that of pure TiO2 electrode. This indicates that there exists a favorable energy level alignment between TiO2 NWs and hollow PbSe NCs. Among them, (Au-PbSe yolk-shell NRs)@TiO2 has the smallest radius in comparison to the other three electrodes. Therefore, it manifests the fastest charge carriers transfer rate. The physics behind this result can be explained by the highly efficient photoexcitation and electron-hole separation (c) Corresponding EIS spectra for four parallel photoanodes with light illumination of λ > 600 nm; (d) Incident photon to current conversion efficiency (IPCE) plots of (PbSe NCs)@TiO 2 and (Au-PbSe yolk-shell NRs)@TiO 2 in the wavelength range 600-1000 nm. The extinction spectra of PbSe and Au-PbSe yolk-shell NRs sensitizers are also shown.
To understand the enhanced mechanism of photocurrent response in the sensitized TiO 2 NWs photoanodes, the processes of inner charge transferring are further discussed in Figure 7. As we know, apart from the irradiance on the electrode, the photocurrent response depends on the light-harvesting efficiency, the yield for electron injection, and the charge collection efficiency. In our research, since the electron scavenger is absent in the electrolyte and sufficiently positive potential, the photocurrent is mainly determined by the light-harvesting efficiency and the yield of electron injection. Firstly, the Au-PbSe yolk-shell hybrid NRs with transverse hollow shells possess a stronger T-SPR band in the visible region than the other plasmonic nanostructures, co-operated with the large optical coupling interface, which are more benefit for the light harvesting and utilization in the visible bands. Secondly, a proper energy level alignment at heterojunction between TiO 2 and PbSe can also be achieved by adjusting the proper PbSe shell thickness due to the strong quantum confinement effects, which facilitates the electron transfer from PbSe to TiO 2 [58]. Meanwhile, considering the Fermi level of Au and the Schottky barrier at the Au-PbSe interface, the hot electrons (1.26 eV) derived from the excitation of SPR of Au NRs in Au-PbSe NRs have sufficient energy to surmount the Schottky barrier (≈0.37 eV), so they are injected into the conduction band of PbSe shell [59]. Furthermore, after the hot electrons pass through the PbSe nanobridge at the end of hybrid NRs, they will be drained into the TiO 2 electrode, and transmit to counter electrode through the extra circuit to drive water-splitting reactions. In addition, the hollow and porous nanoshells not only maintain the independence of the plasmon nanostructures, but also provide a channel for the connection between the Au core and the solution. It facilitates hot holes rapidly eliminating by the hole scavengers and recycle the photoreduction/oxidation reactions. PbSe as a fascinating semiconductor material with a large exciton Bohr radius, high index of refraction and multiple-exciton generation [60,61], more interesting studies are under way on the synergistic properties of hollow Au-PbSe hybrid nanostructures.
photoanodes, the processes of inner charge transferring are further discussed in Figure 7. As we know, apart from the irradiance on the electrode, the photocurrent response depends on the light-harvesting efficiency, the yield for electron injection, and the charge collection efficiency. In our research, since the electron scavenger is absent in the electrolyte and sufficiently positive potential, the photocurrent is mainly determined by the light-harvesting efficiency and the yield of electron injection. Firstly, the Au-PbSe yolk-shell hybrid NRs with transverse hollow shells possess a stronger T-SPR band in the visible region than the other plasmonic nanostructures, co-operated with the large optical coupling interface, which are more benefit for the light harvesting and utilization in the visible bands. Secondly, a proper energy level alignment at heterojunction between TiO2 and PbSe can also be achieved by adjusting the proper PbSe shell thickness due to the strong quantum confinement effects, which facilitates the electron transfer from PbSe to TiO2 [58]. Meanwhile, considering the Fermi level of Au and the Schottky barrier at the Au-PbSe interface, the hot electrons (1.26 eV) derived from the excitation of SPR of Au NRs in Au-PbSe NRs have sufficient energy to surmount the Schottky barrier (≈0.37 eV), so they are injected into the conduction band of PbSe shell [59]. Furthermore, after the hot electrons pass through the PbSe nanobridge at the end of hybrid NRs, they will be drained into the TiO2 electrode, and transmit to counter electrode through the extra circuit to drive water-splitting reactions. In addition, the hollow and porous nanoshells not only maintain the independence of the plasmon nanostructures, but also provide a channel for the connection between the Au core and the solution. It facilitates hot holes rapidly eliminating by the hole scavengers and recycle the photoreduction/oxidation reactions. PbSe as a fascinating semiconductor material with a large exciton Bohr radius, high index of refraction and multiple-exciton generation [60,61], more interesting studies are under way on the synergistic properties of hollow Au-PbSe hybrid nanostructures.

Conclusions
In summary, we have proposed a facile and common route to controlled synthesize Au-PbSe hybrid nanostructures. Based on the as-prepared Au-PbSe NRs, we have investigated the growth kinetics of hybrid nanostructures. Under the combined action of Kirkendall effect and the

Conclusions
In summary, we have proposed a facile and common route to controlled synthesize Au-PbSe hybrid nanostructures. Based on the as-prepared Au-PbSe NRs, we have investigated the growth kinetics of hybrid nanostructures. Under the combined action of Kirkendall effect and the Gly-guiding cation transport, morphology modulation from longitudinally (dumbbell-like) to transversely (yolk-shell) symmetric overgrowth of shells on Au NRs are achieved, by simply adjusting the initial Pb 2+ concentration. Interestingly, the plasmonic absorption enhancement with different resonance modes could be tuned by the symmetric distribution of shell on Au NR in our experiments. That provides an effective pathway for maneuvering plasmon-exciton in metal-semiconductor hybrids. In addition, shell-symmetry-dependent photoelectrochemical properties were also observed in Au-PbSe hybrid NRs sensitized TiO 2 electrodes. The TiO 2 NWs electrode sensitized with transversely symmetric Au-PbSe yolk-shell NRs exhibited superior photoactivity over the others, which is attributed to the synergism between effective plasmonic enhanced sunlight harvesting and highly efficient interfacial charge transfer in the hybrid nanostructure. As a versatile method, employed Au@Se nanostructures and Gly[M n+ ] (M n+ = Cd 2+ , Bi 3+ and Cu 2+ ) as reaction precursors, the well-defined Au-CdSe, Au-Bi 2 Se 3 and Au-CuSe hybrid nanostructures were further obtained with our amino acid guiding strategy. We believe that this study could be extended to the fabrication and functionalization of multicomponent nanostructures with controllable morphology and component distribution. Our findings would boost the development of materials for solar energy conversion.
Supplementary Materials: The following are available online at http://www.mdpi.com/2079-4991/10/3/564/s1, Figure S1: Low magnification TEM images of the products obtained at different reaction time for synthesis of yolk-shell Au−PbSe NRs, Figure S2: The average shell thicknesses of Au@Se NRs were respectively 4.2 nm and 11.3 nm. When 20 µL of 0.1 M lead acetate solution was added, the obtained Au-PbSe NRs kept yolk-shell nanostructure, the average thicknesses of PbSe shells were 4.3 nm and 8.5 nm, and the corresponding nanovoid sizes were about 0.4 nm and 4.8 nm respectively, Figure S3: TEM images of (a) Au-CdSe NRs, (b) Au-Bi 2 Se 3 NRs and (c) Au-CuSe NRs. (d-f) Corresponding HRTEM images at the ends of hybrid NR, (g) EDS spectra of Au-CdSe NRs and AuBi 2 Se 3 NRs, (h) XRD patterns of Au-CdSe NRs, Au-Bi 2 Se 3 NRs and Au-CuSe NRs. The standard patterns of hexagonal-phase CdSe (PDF#08-0459), Bi 2 Se 3 (PDF#33-0214) and CuSe (PDF#20-1020) are also displayed, Figure S4: TEM images of Au-PbSe yolk-shell (a) nanocubes NCs and (b) triangular nanoprisms prepared by the same method, Figure S5: (a) Simulated extinction spectra of Au NR, Au-PbSe dumbbell-like and yolk-shell NRs with different symmetric hollow shells; (b) Local field distributions for these three nanostructures at their T-SPR and L-SPR peaks, Figure S6: Corresponding TEM images of three sensitizers (a) hollow PbSe NCs; (b) Au-PbSe dumbbell-like and (c) yolk-shell NRs, Figure S7: Absorption spectra of pristine TiO 2 , (PbSe NCs)@TiO 2 , (Au-PbSe dumbbell NRs)@TiO 2 and (Au-PbSe yolk-shell NRs)@TiO 2 , Figure S8: SEM image of TiO 2 NWs photoanodes sensitized with Au-PbSe yolk-shell NRs, Figure S9: Photocurrent density-applied potential characteristics under illuminations of (a) white light and (b) the light at λ > 600 nm, Table S1: The addition amount of reaction precursors are shown in the table respectively for synthesizing sensitizer of four parallel photoanodes.