Surface plasmons are coherent electron oscillations behaving as localized and propagated modes in metal nanoparticles and nanowires, respectively. In this chapter, we first review some of the applications made in plasmonics with gold nanorods/nanospheres and silver nanowires. For gold nanoparticles with a size of 1–100 nm, the surface plasmons are confined around the particle surface as localized modes to enhance the near-field. For diameter of around 200–300 nm silver nanowires with a length up to 10 μm, the surface plasmons can propagate along the nanowires as waveguide modes to guide the plasmons. We then describe some novel results with regarding to gold nanorod enhanced light emission, silver nanowire supported plasmonic waveguide, gold nanosphere mediated whispering-gallery-mode emission, and energy conversion in silver-polymer plasmonic nanostructures. The work of this chapter highlights the applications of metal nanoparticles and nanowires in plasmonic waveguides to achieve optical energy generation, propagation, and conversion.
- surface plasmon waveguides
- metal nanoparticles
Plasmonics has the fascinating ability to localize and guide light wave at the deep sub-wavelength scale, becomes an inter-discipline merging photonics with electronics [1, 2, 3, 4, 5, 6]. Surface plasmons are free electron oscillations induced by optical methods at the metal surfaces. Both localized and propagated surface plasmons excited in metal nanoparticles and nanowires are of great interest. They not only break the diffraction limit but also allow to guide light in various geometries such as 90° bending . This promises the scaling of optical devices down to the diffraction limit for miniaturized photonic circuits. The localized surface plasmons have the functionality to scatter, absorb and squeeze light into nanometer scale, providing large enhancements of local near-fields . It holds the potential applications in data storage, light energy generation, sub-wavelength optics, nano-optical tweezers, biophotonics and nanoscopy [8, 9, 10, 11]. Gold nanoparticles with sphere/rod shapes and size below 100 nm are highly investigated for many useful applications, such as non/radiative enhancement of nano-crystals , inter-particle coupling effect , single particle plasmon spectroscopy [14, 15, 16], plasmonic sensing [17, 18, 19], plasmonic photocatalysis [20, 21, 22], and so on. Different from the localized surface plasmons of individual nanoparticles, the propagated surface plasmons existing at flat/curved surfaces in metallic planes, films, and wires also exhibit intriguing plasmonic phenomena . The propagation length of surface plasmon modes is inevitably limited by metallic absorption, could also be strongly confined in the lateral section normal to propagation direction. This implies that plasmonic waveguides could transport larger bandwidth of information than that of conventional photonic waveguides. However, there is a trade-off between propagation loss and mode confinement in plasmonic waveguides . To balance this trade off, an alternative method by seamlessly integrating photonic waveguides into plasmonic waveguides can be used . Silver nanowires usually act as plasmonic waveguides with lateral size of 200−300 nm and axial length up to 10 μm, exhibiting many interesting applications. For example, plasmonic interference , wave-particle duality , remote excitation of Raman scattering [28, 29, 30], long-distance plasmonic gain [31, 32, 33], broadside nano-antennas , etc. It is impossible to introduce every result on plasmonics in this short chapter. In the following sections, we will specifically describe some novel results with gold nanorods/nanospheres and silver nanowires for achieving optical energy generation, propagation, and conversion.
2. Localized surface plasmon in gold nanorods
Metal-enhanced fluorescence can be realized via the resonant coupling with localized surface plasmon in metallic nanoparticles, nanorods, and nanostructures [35, 36, 37, 38, 39, 40]. Different form two-dimensional films and/or three-dimensional solutions, metal-enhanced fluorescence in one-dimensional waveguides could provide a lower power consumption and higher density integration for plasmonic circuits. Herein, we describe a novel result of gold nanorod enhanced light emission, which is realized by embedding gold nanorods into polymer photonic waveguide doped with quantum dots at low concentration.
To study plasmonic properties, a single plasmonic waveguide was placed on MgF2 substrate with refractive index (
To clearly examine the distributions of gold nanorods and quantum dots embedded in the plasmonic waveguide, both a bright-field transmission electron microscope (TEM) and an energy dispersive X-ray spectroscopy (EDS) were simultaneously performed. Figure 1c shows EDS spectrum of a plasmonic waveguide while the inset shows the corresponding TEM image. The EDS spectrum verifies the existence of Au (9.43 wt%), Cd (0.02 wt%), Se (0.40 wt%), Zn (0.69 wt%), and S (1.00 wt%) elements. They came from gold nanorods and CdSe-ZnS core-shell quantum dots. The embedded concentrations for gold nanorods and quantum dots are estimated to be of 4 μm−3 and 3.2 × 103 μm−3, respectively.
Figure 1d shows the light emission efficiency at positions A to E (with gold nanorods) and positions A1 to E1 (without gold nanorods). At position B, the emission enhancement is maximized, where plasmonic wavelength overlapped with emission wavelength of quantum dots . The mechanism for emission enhancement can be interpreted as follows: (1) by coupling a 473-nm blue light into plasmonic waveguide, the embedded quantum dots are photo-excited and then emit 600-nm red light. (2) The emitted 600-nm red light excites the localized surface plasmon of gold nanorods, which leads to an enhancement of local near-field. (3) The enhanced local near-field increases the stimulated radiative decay rate of quantum dots, thus leading to the increasing of quantum yields and the decreasing of fluorescence lifetime .
In fact, emission quenching could happen because free electrons can transfer from quantum dots to gold nanorods once they are closely contacted. For instance, emission quenching of quantum dots by gold nanoparticles has been previously reported [44, 45]. As shown in Figure 1a, the locally enhanced inhomogenously distributed emission spots can be explained by the unevenly-increased in the local density of plasmonic sates around gold nanorods. This inhomogeneous can be improved by linking quantum dots and gold nanorods via chemical/biological coupling to ensure their efficient interactions. In any case, the total emission efficiency depends on the quantum yield, self-absorption of quantum dots, resonance properties of localized surface plasmon in gold nanorods, and propagation loss of the plasmonic waveguide.
For the measurements of emission intensity, the dark-field optical microscope images with RGB modes were transformed into gray levels employing software (Adobe Photoshop), and the gray values were summed up to acquire the normalized intensity, this method was previously reported . The yellow rectangular in Figure 1a and b is taken as the sum-up region with an area of 21 × 18 μm2. Figure 1e shows the normalized intensity of red emission along the plasmonic waveguide (red line) and photonic waveguide (green line) as a function of propagation distance. It indicates that the existence of gold nanorods seriously affects the propagation distance of plasmonic waveguide, which is due to the larger scattering loss. In addition, some local regions with non-uniform particle density, refractive index, and crystalline would give rise to bulk scattering in the plasmonic waveguide.
3. Propagated surface plasmon in silver nanowires
Silver nanowires possess sub-wavelength mode confinement and low propagation loss, but the couple of light into such small nanowires are extremely challengeable. For this challenge, several methods to light coupling have been proposed, including: (1) total internal reflection method utilizing an optical prism to compensate for momentum mismatch between photon and surface plasmon ; (2) localized excitation method via focusing laser beam directly on a scattering center of silver nanowires [48, 49]; and (3) near-field coupling method using optical dipole with large momentum components to match that of surface plasmon, where quantum emitters usually located in the near-field of silver nanowire [50, 51]. However, above three coupling methods cannot easily interconnect silver nanowires with photonic waveguides for nanophotonic circuits. Herein, we describe a novel result of silver nanowire supported plasmonic waveguide by coupling photons from quantum-dot-doped nanowire.
A scanning electron microscope (SEM) micrograph of one silver nanowire with a diameter of 300 nm was interconnected with a quantum-dot-doped nanowire with a diameter of 800 nm at an angle of 60° is presented in Figure 2a. To inspect this crossing angle in better detail, an enlarged view is given in Figure 2b. For more practical device applications, the interconnection of more than one silver nanowire with a same quantum-dot-doped polymer nanowire is extremely desirable. For example, Figure 2c presents an SEM micrograph of silver nanowires 1 and 2 with the same diameters of 300 nm were interconnected with a quantum-dot-doped nanowire (800-nm in diameter) at angles of 60 and 65°, respectively. The mutual distance between silver nanowires 1 and 2 is about 6.4 μm. To realize hybrid interconnection with high-density of plasmonic and photonic nanowires, more than three silver plasmonic nanowires with distinct lengths and diameters would be interconnected with the same quantum-dot-doped photonic nanowire at distinct angles and intervals, which could provide versatile multi-functionalities in nanoscale circuits [52, 53].
Optical characterization of the silver nanowires was performed under an optical microscopy using a micro-spectrophotometer (CRAIC, 20/20 PV, USA). Figure 3a shows a reflection-type optical microscope image of silver nanowires 1 and 2 with the same diameters of 300 nm was interconnected with an 800-nm diameter quantum-dot-doped nanowire at angles of 57 and 80°, respectively. The lengths of silver nanowires 1 and 2 are about 5 and 4 μm, respectively, and the mutual distance between them is of 10 μm. Figure 3b gives a scattering-type micrograph under dark-field for the crossing structure in Figure 3a illuminated by a beam of 532-nm laser at an optical power of 10 mW. The scattering position J0 comes from individual defects in the quantum-dot-doped nanowire. The larger scattering positions J1 and J2 come from the photonic-plasmonic junctions formed with the silver and quantum-dot-doped nanowires . In the photonic-plasmonic junctions, when the surface plasmon of silver nanowires were launched by photoluminescence from quantum-dot-doped nanowire. Among the launched plasmonic modes, the dominant mode is longitudinal mode and the produced resonance could have Fabry-Perot characteristics . The smaller scattering positions S1 and S2 come from the end tips of the silver nanowires, where the propagated surface plasmons were converted into free space photons.
The two silver nanowires with same diameters of 300 nm can strongly confine the 580-nm photoluminescence into sub-wavelength scale dimensions, giving rise to their relatively compact interconnection with the quantum-dot-doped nanowire. For briefness, the photoluminescence spectra collected at positions J0, J1, J2, S1, and S2 were plotted in a single graph as Figure 3c. The peak wavelengths for positions J0, J1, J2, S1, and S2 are 580, 585, 590, 595, and 605 nm, respectively. The inset image of Figure 3c shows surface plasmon propagation in the silver nanowires and emitted photon propagation in the quantum-dot-doped polymer nanowire. The quantum-dot-doped nanowire produced distinct colors of yellow, yellow-orange, and orange from positions J0, J1, and J2, respectively. This phenomenon is called “wavelength-converted waveguiding”, which also previously observed in dye-doped polymer nanofiber . The color difference between yellow-orange (J1) and red-orange (S1) in silver nanowire 1 comes from the metallic loss induced energy dissipation, and the resulted peak wavelength changed from 585 to 595 nm. Similarly, the colors are different between orange (J2) and red (S2) in silver nanowire 2, and the peak wavelength changed from 590 to 605 nm. This is a frequency-dependent dispersion effect in these two silver nanowires .
Another novel result is optical routing in single silver nanowires . Semiconductor micro-ribbon and silver nanowires were assembled to realize routing structure, as shown in SEM micrograph of Figure 4a. One silver nanowire was sitting on top of a semiconductor SnO2 ribbon, and a second silver nanowire just cling to it with a 12 μm overlapping. The three color arrows show the end tips of the silver nanowires, and the Inset shows the enlarged view of the overlapping region. The surfactants on the silver nanowires have already been cleared so that the two silver nanowires were contact directly. Figure 4b and c show the intensity mapping and real-color micrograph of the optical routing from semiconductor SnO2 ribbon photoluminescence. Surface plasmons were launched into the first silver nanowire in the silver-SnO2 overlapped region, and evanescently coupled into the second silver nanowire with low scattering loss in the silver-silver overlapped region. This efficient coupling in the silver-silver region is benefited from the large surface plasmon mode overlaps due to the closely contact between the nanowires. Interestingly, the relationship of the end tip emission color with propagation distance on the case of single silver nanowire was also investigated. Figure 4d–4f individually display the red, green, and blue color panel of the real-color micrograph in Figure 4c. The closer the propagation distance, the emission composes more short-wavelength components. The blue-wavelength components just exist at the first silver nanowire tip with a propagation distance of 8 μm, while the green-wavelength components survived 20 μm of propagation and the red-wavelength components were the only visible one with propagation distance up to 40 μm.
4. Plasmonic nano-cavity in gold nanospheres
Different from dielectric micro-cavities, plasmonic nano-cavities could confine light into the nanometer scale mode volume [60, 61]. Optical investigations based on circular nano-cavities are extremely interesting due to the whispering-gallery-modes, which are attributed to the total internal reflection of light at the plasmonic interface along the equator. Herein, we describe a novel result of whispering-gallery-mode emission in plasmonic nano-cavity, which combines gold nanosphere and quantum dots by using electrostatic attraction. Figure 5a shows polarization-dependent photoluminescence intensity of the emitted light. The dependence can be described by a sinusoidal function. The minimum (−90°) and the maximum (10°) photoluminescence intensities are corresponding to perpendicular and parallel to the extinction direction of the gold nanosphere, respectively. The period of 180° is similar to that reported in quantum dots on gold nanodiscs .
Figure 5b shows the emission spectrum containing five narrow bands, which indicates the characteristic of the whispering-gallery-modes. The maximum peak of whispering-gallery-mode is well coincidence with that of solution photoluminescence. Meanwhile, the optical feedback is strong enough to resist the plasmonic loss. Figure 5c shows the photoluminescence spectra of 800 and 550 nm diameter quantum-dot-coated gold nanosphere producing the several narrow bands, while the maximum peaks towards to short wavelength range as diameter increasing. This phenomenon is governed by changing in whispering-gallery-mode states density and the near-field coupling strengths. Figure 5d shows the photoluminescence decay spectra of quantum-dot-coated gold nanosphere (blue) and the quantum dots solution (red). They are multiple-exponential process, including intrinsic decay, plasmonic quenching, and plasmonic enhancement. The lifetimes were calculated from 1/
Molecular emitters located in a plasmonic nano-cavity experience an intriguing process to be coupled into the surrounding optical field . Cucurbit(7)uril is hydro-soluble and can encapsulate only one molecule of methylene-blue inside it. Encapsulation of methylene-blue inside cucurbit(7)uril is verified by absorption spectroscopy analysis (Figure 6a): methylene-blue dimmers (with characteristic ‘shoulder’ of small peak at 625 nm on the red solid curve) disappear when mixing low concentrations of methylene-blue into cucurbit(7)uril (Figure 6a, blue solid curve). Contrast experiments use the smaller molecule of cucurbit(5)uril also have this shoulder peak (red dashed curve), eliminating the possibility of parasitic binding. Encapsulating single molecules of methylene-blue into cucurbit(7)uril can be used to avoid molecular aggregation. Carboxide portals at either end of the 0.9-nm in height cucurbit(
Another novel result shows that 44-nm in diameter nanospheres with a gold core and dye-doped silica shell can be used to overcome the plasmonic loss with optical gain and realize a stimulated emission of surface plasmons . Figure 7a shows a nanosphere with a gold core, supporting for localized surface plasmon modes, and coated by a silica shell doped with organic dye OG-488 (Oregon Green 488), supporting for optical gain. TEM and SEM measurements show the diameter of gold core and the thickness of silica shell are about 14 and 15 nm, respectively (Figure 7b and c). The molecule number of dye per nanosphere was estimated to be about 2.7 × 103, and the nanosphere concentration in suspension was about 3 × 1011 cm−3. The calculation of plasmonic laser mode (Figure 7d) obtains the stimulated emission wavelength (
5. Plasmonic conversion in silver-polymer nanostructures
Organic polymers with extraordinary properties to incorporate with laser dyes for providing optical gain over broadband visible spectrum, which makes them potential for tunable full-color lasers [67, 68]. Meanwhile, the mechanical flexibility of polymers allows to integrate them with metallic nanostructures, confining light into a small mode volume by surface plasmon . In addition, flexible polymers have an outstanding function to self-assemble into optical micro-cavities with high-quality, where propagated light beam will be continuously confined via total internal reflection. Consequently, the large evanescent field around the air-cavity interface results in efficient conversion between photon and surface plasmon . Herein, we describe a plasmonic conversion to obtain sub-wavelength output of full-color lasers in a silver-polymer heterostructure . Figure 8a shows the assemble process of PS and dye molecules via dropping a defined amount of water into the PS-dye blend solution. During the nucleus formation of PS, the powerful π-π interaction makes the dye molecules slowly diffuse into the PS matrix. Once the solvent was evaporated, the silver-polymer microdisks with dyes can be successfully fabricated. Four organic dyes, trans-DPDSB, C153, CNDPASDB, and HMDMAC, with emission colors across the full visible spectrum, were intentionally selected for optical gain media. Under ultraviolet (330–380 nm) excitation, the silver-polymer microdisks emitted homogenous blue (b), cyan (c), green-yellow (d), and red (e) colors, respectively (Figure 8b–8e). Importantly, the full colors were outputted with the sub-wavelength silver nanowire at end tips (white circles). This demonstrates the typical feature of surface plasmon waveguide, and the plasmonic conversion at the silver-polymer connections.
Another novel result of energy conversion between photonic nanowire and plasmonic nanowire will be described . The photonic nanowire is CdSe-ZnS core-shell quantum dots doped polymer nanowire, and the silver nanowire served as plasmonic nanowire. The conversion efficiency is about 32%, which is realized by the Förster resonance energy transfer. Figure 9a shows SEM micrograph of quantum-dot-doped photonic nanowire were interconnected with silver plasmonic nanowire at a crossed angle of 45°. Once the plasmonic and photonic nanowires are directly contact, the surface plasmon field and evanescent field around photonic nanowire would overlap, leading to efficient conversion from photon to plasmon at the coupling area . Figure 9b gives the dark-field optical micrograph of the silver-polymer crossed structure with red emission. The silver nanowire is about 55 μm in total length, and the lengths of the long (white arrow) and short (yellow arrow) regions on the two side of the photonic nanowire (refer as ‘limbs’) are 40 and 10 μm, respectively. The plasmonic conversion can be understood by the energy transition: photon-exciton-plasmon, and not need to match momentum, because the dipolar near-field of quantum dots has momentum components matching that of surface plasmon. Hence, the crossed angle cannot influence the plasmonic conversion efficiency . The exponential decay curves of Figure 9c and d indicate surface plasmon propagation lengths of 10 and 5 μm for long and short limbs, respectively. In addition, Figure 9e gives the emission spectra collected at coupling area, two distal ends of long and short limbs with wavelength centered at 650, 660, and 654 nm, respectively.
In this chapter, we have briefly introduced some important applications with localized and propagated surface plasmons in gold nanospheres/nanorods and silver nanowires. Specifically, we have described some novel results on gold nanorods enhanced light emission, surface plasmon propagation in silver nanowires, gold nanosphere as a plasmonic nano-cavity, energy conversion in silver-polymer nanostructures. Due to the limited space, many important progress in quantum plasmonics, nonlinear plasmonics, and photovoltaic plasmonics cannot be described altogether. The work in this chapter presents the applications of gold/silver nanoparticles/nanowires in nanophotonics to realize light generation, propagation, manipulation and conversion. It is an ultimate dream for plasmonics to combine photonics and electronics on practical devices and circuits. This huge challenge continued to motivate the research interests all around the world.
We thank the supports provided by National Natural Science Foundation of China (Grant 21703083), the Natural Science Foundation of Guangdong Province (Grants 2017A030313026 and 2017A030310463), the Science Research Project of Guangzhou (Grant 201804010468) and the Fundamental Research Funds for the Central Universities (Grant 21617334).
Conflict of interest
The authors declare no conflict of interest.