Noble metal nanostructures supporting surface plasmons arising from the coherent oscillations of the conduction electrons under the radiation of the incident light have been widely investigated 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 . The optical spectral signatures of the plasmonic nanostructures are mainly dependent on the distribution of the electromagnetic field on the surface of the metal nanostructures. When the size of the metal nanostructures is smaller than the wavelength of the incident light, they support localized surface plasmon resonance (LSPR) at particular resonance wavelengths 1 . The LSPR properties of the plasmonic nanostructures are size and shape dependent 1 2 3 . With the increase of the size of the metal nanostructures, high-order resonance occurs owing to the surface plasmon polariton (SPP) mode interferences. For example, metal nanowires support the Fabry-Perot (FP) modes 6 , micron-size metal nanoplates support the whispering gallery modes 7 , and the flag type of metal nanostructure supports competitive LSPR and FP modes simultaneously 23 . These metal nanostructures with regular shapes usually exhibit narrow-band resonance characteristic seen from their extinction spectra.

As well known, on the contrary to those elemental nanoparticles, metal nanostructures with complicated geometries, such as nanochains and branched nanowires assembled or fused by the elemental nanoparticles, show enhanced light-trapping ability 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 . When the metal nanoparticles are in close proximity or jointed together, the intensity of the localized electromagnetic field at the corner area and the junctions of these nanostructures are dramatically enhanced owing to the existing plasmon coupling between different propagation modes or resonance modes 8 9 . It is usually accompanied by obvious redshift and extension of their resonance bands 3 9 . The overall optical properties including obvious light-trapping and scattering enhancement in a wide wavelength range make these complicated metal nanostructures highly desirable in improving the performance of bio-chemical sensors 21 22 , solar cells 24 25 , and wide-bandwidth light-emitting diodes 26 . Although considerable progress has been made in the fabrication methods of such complicated metal nanostructures, such as laser welding 8 9 10 , sintering triggered thermally 11 or chemically 12 , electrodeposition 13 , microwave irradiation 14 , and chemical synthesis methods 15 16 17 18 19 20 21 22 , it is still a challenge to fabricate high-yield metal nanostructures with excellent light-trapping property in a wide wavelength range to meet the practical demands for a large-scale production.

In this study, we present a simple and facile light-induced colloidal method to fabricate high-density branched silver nanowires and nanomeshworks. These complicated nanostructures showed significant light-trapping and scattering properties in the wide range from the visible to the near-infrared wavelengths, arising from the shape-dependent longitude surface plasmon resonance. The broadened bandwidth electromagnetic field enhancement characteristic makes these nanostructures useful in optical processing and photovoltaic applications.

The fabrication process of the branched silver nanowires and nanomeshworks includes two steps.

The color of conventional chemical synthesized silver nanowire solution is pale green accompanied with strong reflection 4 due to the narrow resonance bands and selective light localization properties. Figure 2 shows the typical LSPR spectrum of silver nanowire with smooth surface calculated by three-dimensional finite element method (FEM) 9 27 28 . The silver nanowire supports longitude SPP modes which reflect between its two terminal facets. Therefore, it shows periodic plasmon resonance bands with narrow bandwidth arising from the Fabry-Perot interference of the SPP modes. From the inset in Figure 2, one can see that the electric field is distributed at the surface and the ends of the nanowire. However, light localization and scattering enhancement mainly occur at the ends of the nanowire. Therefore, scattering is not obvious when the SPP modes are transmitted along the nanowires with smooth surface.

Compared with the conventional silver nanowire solution, silver solution prepared in our way containing branched nanostructures shows greatly enhanced light-trapping and scattering characteristics in a wide wavelength range. The two-step light-induced chimerical colloidal method used here was first reported by Pietrobon and Kitaev for the synthesis of decahedral silver nanoparticles 2 . The scheme of the light exposure process is shown in Figure 1a. Surprisingly, silver nanostructures with distinct morphology and optical spectral signatures were found when we increased the material concentration by 100 times higher. Figure 1b shows the extinction spectra of the silver solution measured by a fiber-optic spectrometer (PG2000, Ideaoptics Technology Ltd., Shanghai, China) and the photographs of the solution samples at different exposure times. The first step is the synthesis of the silver seed solution. As shown in the inset of Figure 1b, the color of the diluted silver seed solution (exposure time is 0 h) is light yellow. As shown in the extinction spectrum, a narrow resonance band at 420 nm corresponding to the LSPR wavelength of typical silver nanospheres with a diameter of several nanometers 3 can be observed. The second step is the light-induced regrowth process of the silver nanostructures which is highly dependent on the material concentration. At a low concentration as reported in 2 , decahedral silver nanoparticles with uniform sizes and shapes are the ultimate product. However, when the material concentration was increased by 100 times, the ultimate products containing mainly the branched nanowires and nanomeshworks can be observed. As seen from the extinction spectra, the resonance band at 420 nm decreased, and the absorption ratio in the longer wavelength increased obviously with the increase of the exposure time. As the welded metal nanobranches and nanomeshworks increased, the color of the solution darkened rapidly with the extension of the exposure time, which is shown in the inset of Figure 1b. After a 5-h exposure procedure, the color of the solution turned to black which is obviously different from silver nanoparticles with regular shapes, such as bared nanowires 4 or nanoplates 3 . The optical spectra and the photographs of the solution are strong evidences to show that the ultimate silver nanostructures can trap light effectively in a broad wavelength range from the visible to the near-infrared wavelengths.

In the light exposure process, the small silver seeds aggregated and welded together when the solution was under exposure. The final morphology of the nanostructures depends on the concentrations of the capping agents, PVP, and l-arginine. As discussed in 18 , high PVP concentration serves as a structure-directing agent to keep the nanostructure growth linear. High l-arginine concentration controls the reaction velocity and avoids the size growth of the nanoparticles 2 . Figure 3 shows the transmission electron microscopy (TEM) (Tecnai G2, FEI, Hillsboro, OR, USA) images of the ultimate silver nanostructures after exposure. The TEM samples were washed by ethanol and deionized water and then dispersed uniformly by ultrasonic before measurement. The typical nanostructures include branched nanowires and nanomeshworks. The diameter of these branched nanowires is about several tens of nanometers. Figure 3a,b shows linear branched nanowires with rough surfaces. It was found that there are many knobs and branches in the nanowires. Figure 3c shows nanomeshworks containing many short nanowires connected together randomly in three dimensions. From the high-resolution TEM image in Figure 3d, one can see that the branches have joined together permanently, obviously different from the nanochains assembled by adjacent nanoparticles 17 19 20 .

To investigate the light-trapping property of these nanostructures, we use three-dimensional FEM to simulate the electric field distribution of the branched nanostructures. Rectangular wave incoming from the upper x y plane was set as the source boundary. The other outer boundaries were set as the scattering boundary condition. The cladding layer surrounding the silver nanostructures is water with a refractive index n = 1.33. The dispersion coefficient of water is neglected in the simulation. The dielectric constant of silver is taken from 29 .

We first investigated the optical property of the branched silver nanowires. In the numerical model, we created a branched nanowire with randomly distributed branches and knobs referred to the morphology shown in the TEM images of Figure 3a,b. The configuration of the silver nanowire is shown in Figure 4a,b. The morphologic characteristics are listed as follows: the nanowire is knotty with an average diameter of 30 nm, the distance between the adjacent knobs is approximately 100 nm, the diameter of the knobs is between 30 and 50 nm, the branches connect to the bus nanowire with random angles, and the total length of the nanowire is approximately 800 nm. Figure 4c shows the relationship between the amplitude of the normalized electric field |E| and the wavelength at different positions of the branched silver nanowire including the branch, the corner between two branches, the junction, and the end as labeled by A, B, C, and D, respectively, in Figure 4b. There are many resonance bands covering the wavelength range from the visible to the near-infrared wavelengths in the optical spectra. The bandwidths of the resonance bands are wide, and the amplitudes at the resonance peaks are high, especially at the branches and the corner area. Figure 5 shows the simulation results of the normalized electric field spatial distribution at different z positions seen from the x y plane. The wavelength of the incident light is 940 and 1,020 nm in Figure 5a,b, respectively. Light can be easily localized at the positions of the knobs and the corners between the branches when it propagated along the nanowires with rough surfaces. It leads to various wavelength-dependent ‘hot spots’ 3 21 which are randomly distributed in the nanostructures. The light intensity at the area of the hot spots can be enhanced greatly, leading to a strong interaction of light with matters.

Figure 6 shows the LSPR spectra at different positions distributed in a silver nanomeshwork. The complicated meshwork is formed by randomly distributed short branches in three-dimensional space, as illustrated in Figure 6a,b. The diameter and the length of the short branches were set to be approximately 30 and 100 nm, respectively. In Figure 6c, the three curves represent the normalized electric field |E| at the junction, the branch, and the end of the meshwork highlighted in Figure 6b. The LSPR spectra also exhibit multiple resonance bands with intense light enhancement in a wide wavelength range at the branch and the end area of the nanomeshwork, which is the same phenomenon as the nanowires. However, the light enhancement at the junction area is not obvious. It is because the longitudal resonant cavity length of the nanomeshwork is much shorter than that of the nanowire in our models. For such nanostructures with short resonant cavity length, light is easily be localized at the branches and the corner area rather than the middle area without sharp corners. Figure 7 shows the simulation results of the wavelength-dependent normalized electric field |E| distributions in the silver nanomeshwork at different planes along the z-axis. All images shown so far indicate that the silver nanomeshwork behaves like a three-dimentional ‘light cage’ which traps light at those randomly distributed branches and knobs. The distribution of the hot spots is also wavelength dependent. Such nanostructures can trap light with different wavelengths effectively in large-space areas.

The above simulation results indicate that such randomly constructed silver nanostructures with rough surfaces and multi-branches have high light-trapping efficiency, in accordance with the measured extinction spectra.

In this study, we introduce a simple chemical method for the fabrication of high-density branched silver nanostructures. Both experimental measurement and relative three-dimensional numerical simulation results show that these nanostructures have significant properties as follows: First, these branched silver nanostructures have significant light-trapping and scattering properties in a broad wavelength range. Second, light can propagate in a longer distance along the waveguide-like plasmonic nanostructures to improve the interaction between the surrounding materials and light. Third, the fabrication routes with easy operation and high yields meet the satisfaction of the large-scale production. These properties make such nanostructures useful in practice applications, such as photovoltaics, bio-chemical sensing, and optical processing.

The authors declare that they have no competing interests.

XYZ carried out the main part of synthetic, analytical, and simulation works and drafted the manuscript. SQZ, LDW, and YJS participated in the synthetic and analytical works. TZ, XFL, and QLW participated in the discussion of the experimental details and participated in the draft preparation. All authors read and approved the final manuscript.