Abstract
The research and development of optical metasurfaces has been primarily driven by the curiosity for novel optical phenomena that are unattainable from materials that exist in nature and by the desire for miniaturization of optical devices. Metasurfaces constructed of artificial patterns of subwavelength depth make it possible to achieve flat, ultrathin optical devices of high performance. A wide variety of fabrication techniques have been developed to explore their unconventional functionalities which in many ways have revolutionized the means with which we control and manipulate electromagnetic waves. The relevant research community could benefit from an overview on recent progress in the fabrication and applications of the metasurfaces. This review article is intended to serve that purpose by reviewing the state-of-the-art fabrication methods and surveying their cutting-edge applications.
© 2018 Optical Society of America under the terms of the OSA Open Access Publishing Agreement
1. Introduction
The past decade has witnessed a sustaining wave of interest and effort in developing optical metamaterials that exhibit exotic electromagnetic properties. These metamaterials are typically constructed with subwavelength building blocks that are artificially arranged in 3D configurations. The demonstration of these desired phenomena often times requires light to travel through the 3D structure and one undesirable consequence is always the significant attenuation of light intensity at the output. The strong attenuation is the direct result of the ohmic losses associated with the plasmonic metals typically required for their negative dielectric functions as subwavelength constituents for the fabrication of metamaterials. A viable pathway to circumvent this roadblock is naturally to minimize the penetration depth of the light yet still allowing strong light-matter interaction. This concept was first introduced in 2003 where the term, metafilm, as a 2D category of the metamaterial was brought up [1–3]. The experimental demonstration came about in 2011 [4,5] and since then, the term “metasurface” was widely used in the community. The well-known optical phenomena of reflection and refraction that occur at the interface of two media can be altered with subwavelength elements artificially arranged at the 2D interface. Such metasurfaces operating in either reflective or transmissive mode employ tunable phase discontinuity, resulting in higher efficiency with much less intensity attenuation, because light is not required to propagate through a large distance in order to accumulate sufficient phase change before emerging on either side of the metasurfaces. Another benefit is obviously the simplification in fabrication. Needless to say, the degree of complexity in fabricating 2D structures is orders of magnitude less than those of 3D which has been a major reason why many of the nicely designed optical properties from 3D metamaterials are always hard to realize in practice.
Propelled by ingenuity and innovation from many groups around the world, metasurfaces today have shown great potential for practical applications. Some of the metasurfaces are made of metal structures while others involve only dielectric. Metasurfaces demonstrated in early years were all made of noble metal nanostructures utilizing their plasmonic properties such as multi-resonance, gap-plasmon or hyperbolic dispersion. The first proposed and studied metasurface is of the multi-resonance type involving V-shaped antennas that produce a phase shift covering the range of 0 to 2 [4–7]. However, the low efficiency and weak cross-polarization conversion severely limited its application. The gap-plasmon metasurfaces, on the other hand, use the metal-insulator-metal structure to achieve 2 phase modulation by generating strong near-field coupling between the top antenna array and the bottom metallic plane [8–14]. This type of metasurfaces has the benefit of allowing for strong co-polarization conversion, but can only be used in reflective applications. Hyperbolic metasurfaces possess a metal-like behavior in one direction and a dielectric-like property in the other, supporting surface plasmon polaritons (SPPs) that propagate at the interface between the metal and dielectric [15–19]. The SPP propagation preserves hyperbolic dispersion below a critical wavelength and becomes elliptically dispersed beyond it. One significant benefit is its ability to induce strong field confinement due to the high local density of states for the SPPs as demonstrated in hyperbolic metamaterials.
These metasurfaces typically operate in reflective mode because their transmission efficiency is low due to the strong metal loss. In order to achieve high transmission, all-dielectric metasurfaces have emerged and are rapidly gaining momentum [20–27]. These metasurfaces are constructed of 2D patterns of near-wavelength dielectric structures on a flat surface. One such type is of Huygens featuring electric and magnetic dipole resonances that are spectrally overlapped with comparable strength capable of phase modulation of 0 to 2 and near-unity transmission [28–30]. Metasurfaces of this type comprise of aperiodic or multilayered structures in order to engineer surface impedance to minimize reflection. Their transmission efficiencies in the microwave and near-infrared regimes are high but deteriorate rapidly at visible frequencies. The other type is the so-called high-contrast metasurfaces consisting of 2D dielectric arrays of high refractive-index contrast that allow for excitation of quadrupoles and high-order multiples in addition to electric and magnetic dipoles [31–33]. The dielectric nanostructures in such metasurfaces act as truncated waveguides that strongly concentrate optical energy around the nanostructures. The advantage of the high-contrast metasurfaces is the ability to exhibit high diffraction efficiencies over a broad range of steering angles of incident light.
The Pancharatnam-Berry metasurfaces are primarily developed for their strong ability to realize full-phase control of circularly polarized light [34–39]. The mechanism for phase control is provided by rotating the orientation of the nanostructures of identical dimensions in the 2D plane instead of adjusting the geometry of nano-resonators that are employed in the aforementioned metasurfaces. Such metasurfaces follow simple design rules and are capable of broadband operation but limited only to the circularly-polarized incident light.
There is yet another type of metasurfaces synthesized by depositing a highly absorbing ultrathin film on a substrate whose purpose, quite different from all the above, is to fully absorb incident light over a broad spectrum [40–45]. These thin-film metasurfaces do not require any specific patterning of nanostructures and the perfect absorption occurs when the difference in complex refractive indices between the film and substrate is properly chosen. Other thin-film metasurfaces have been applied to ultrathin nano-structural coloring [46], broadband reflectors [47] and absorbers [48], polarization beam splitters, converters and analyzers [49], as well as superchirality [50].
There have been several excellent review papers focusing on metasurfaces of different kinds and functionalities [51–67]. In this review article, we choose to review recent progress made in fabricating these optical metasurfaces and survey their cutting-edge applications.
2. Fabrication techniques for metasurfaces
In this section, we begin to review various methods and technologies developed for the fabrication of optical metasurfaces. These methods can be generally classified into four categories as shown schematically in Fig. 1. Three of them are well-established fabrication methods: direct-write, pattern transfer, and hybrid patterning lithography. The fourth is the so-called alternative techniques that only began to emerge as fabrication methods for metasurfaces. These four categories are primarily employed to produce passive optical metasurfaces. For actively tunable metasurfaces, however, novel fabrication methods need to be developed.
2.1 Direct-write lithography
As one of the most matured technologies developed and adapted in semiconductor manufacturing, photolithography should also be one of the most promising technologies for optical metasurface fabrication considering its advantage in high yield, large area and large volume mass production. Traditional photolithography uses light to go through a focusing lens in order to transfer a geometric pattern from a photomask to a light-sensitive chemical “photoresist”. Shorter-wavelength light sources are preferred in fabricating the optical metasurfaces with fine features, and such sources are known to cause damages to the lens and mask. To circumvent this technical difficulty, the maskless direct-write lithography has been developed (Table 1) which includes three different methods employing either particle beam, mechanics or laser to pattern nanostructures.
2.1.1 Particle beam lithography
Particle beam lithography uses a focused Gaussian particle beam to generate a highly concentrated spot being exposed to one pixel at a time. Two well-established particle beam methods for the fabrication of optical metasurfaces are electron-beam lithography (EBL) and focused-ion-beam (FIB) lithography. EBL along with subsequent pattern transfer techniques can be roughly categorized into either bottom-up or top-down approach depending the way with which the nanostructures are made. The bottom-up approach employs the evaporation or deposition of atoms or molecules together with the lift-off process to build up nanoscale structures, while the top-down refers to creating nanostructures by using the etching process.
Our group has developed a bottom-up approach that produced a broadband optical metasurface operating in the infrared region [68] as shown in Fig. 2(a). The process starts with coating a resist layer on a substrate followed by exposing the concentrated electron beam directly onto the top surface of the resist-coated substrate. The subsequent process builds up the nanostructures by evaporating atoms after developing the exposed resist-coated substrate. Figure 2(b) is the top-view of the scanning electron microscope (SEM) image of an optical metasurface after the lift-off process. In a parallel approach, our group also reported using a top-down method to fabricate the optical meta-lens as illustrated in Fig. 2(c) [69]. It begins with the spin-coated resist layer being exposed to the electron beam followed by an etching process to reduce its lateral dimensions to form the nanostructures. The top-view of the SEM image of the optical meta-lens is shown in Fig. 2(d). Challenges of EBL for large-scale manufacturing are its high cost and low speed operation that requires a highly stable environment. The resolution of EBL is limited by the electron scattering in the resist due to the proximity effect [70–72].
FIB lithography is a one-step etching process in which a beam of ions instead of electrons mills the sample surface via a sputtering process with nanometer precision. This process becomes more powerful when it is equipped with the SEM function to form the so-called dual-beam system. With this system we can simultaneously observe and mill the sample surface at any designated spot facilitated by direct visualization. Figures 3(a) and 3(b) show SEM images of the FIB-fabricated metasurfaces for visible hologram and optical vortex generation and focusing [73,74]. FIB lithography is unsuitable for large-area manufacturing because of high cost and low throughput. In addition, it faces fabrication challenges such as aspect ratio limitation, ion doping, long milling time that leads to spatial drift of sample images, and sample damage during imaging and milling.
2.1.2 Probe scanning lithography
The probe scanning lithography (PSL) is another technique used in nanofabrication. Its ultimate resolution is reached by employing the technique of atomic force microscopy (AFM). It utilizes a probe to scratch out nano-patterns in resist or to arrange nano-particles in patterns. Figure 3(c) shows the surface morphologies of the negative refractive index metasurfaces in mid-infrared, fabricated by the PSL under normal atmospheric pressure, at room temperature and humidity [75]. The main problem of AFM-based PSL is its poor aspect ratio — “scratches” are relatively wide and shallow. Other techniques such as scanning tunneling microscope (STM) and scanning near field optical microscope (SNOM) are developed to solve the problem of poor aspect ratio. However, all of them are low throughput and expensive. Further improvement of PSL is necessary for large area patterning in order for it to be used in large-scale manufacturing.
2.1.3 Laser lithography
It is obviously desirable to develop large-area fabrication techniques with better flexibility, high precision and good uniformity. There are two maskless laser-based approaches that are capable of rapid and low-cost processing of micro- and nanostructures: laser-direct-write (LDW) lithography and laser-interference lithography (LIL).
The LDW lithography utilizes computer-controlled optics to project the desired nano-patterns directly onto the photoresist by holding the mask in software. It not only enables nano-fabrication of materials that are hard to machine mechanically but also generates 3D surface profiles by writing with variable laser dosage. As a result, the phase noise generated by discrete systems can be suppressed through the use of a continuously shaped metasurface [Fig. 3(d)] [76]. The LDW lithography effectively offers a compromise between the feature size and processing cost. One drawback of this method is that it is not a batch process.
The idea of LIL based on the interference of two or more coherent laser beams was put forward to produce large-area periodic nanostructures. As shown in Fig. 3(e), the metasurface acting as a linear polarization converter composed of ellipse-shaped plasmonic planar resonator can be fabricated by two-beam LIL [77]. Advanced LIL with multiple exposures and non-co-planar beams can produce complex periodic nanostructures [79]. As illustrated in Fig. 3(f), a metasurface composed of 2D complex nanostructures is realized by an orthogonal LIL to achieve a broadband and high-efficiency reflective linear polarization converter [78]. Indeed, LIL is a large-area, high-efficiency, inexpensive, maskless technique - a batch process that is limited to periodic patterns only.
2.2 Pattern transfer lithography
Pattern transfer lithography is developed in order to meet the requirements for high throughput and large area fabrication (Table 2). Several techniques that fall into this category are discussed here including plasmonic, nano-imprint and self-assembly lithography.
2.2.1 Plasmonic lithography
It is well known that the resolution of traditional photolithography suffers from diffraction limit. Plasmonic lithography has been developed to acquire deep subwavelength resolution beyond the diffraction limit. A dielectric spacer layer is sandwiched between the photomask with subwavelength nanostructures and the photoresist-coated substrate. Normal incident light excites free-electron oscillations at the interface between metal and dielectric, resulting in SPPs. The SPP waves are capable of confining optical fields in a scale that is much smaller than the wavelength of incident light. When they are used as light source to expose the photoresist-coated substrate, finer features of subwavelength can be achieved. Schematic of the reflective plasmonic lithography structure with a silver lens is illustrated in Fig. 4(a) and SEM image of the anisotropically-arrayed nano-slot metasurfaces fabricated with the technique [80] is shown in Fig. 4(b). The drawback of such plasmonic lithography is that the range of SPP propagation distance of is small because of the metal loss. A superlens is thus placed underneath the mask to improve the efficiency of projection onto the photoresist through the mask. This superlens-embedded plasmonic lithography bends light into a negative angle with respect to the normal direction of the surface due to the negative index of the superlens. Further improvement in resolution has been sought after from the superlens-based plasmonic lithography for the fabrication of metasurface holograms as shown in Figs. 4(c) and 4(d) [81]. Although plasmonic lithography has the benefit of being high throughput and low cost, mass production that requires large-area photomask remains an issue.
2.2.2 Nano-imprint lithography
Nano-imprint lithography (NIL) is a technique that uses mechanical deformation to replicate nanostructures. Conventional NIL employs heat, called thermal NIL, to cure a polymer-coated substrate while a nano-structural master mold is being pressed against the substrate. After the mold is detached from the substrate, the imprinted pattern is transferred onto the polymer layer. Thermal-NIL has been used to fabricate ultrathin polarizing plasmonic metasurfaces [Fig. 5(a)] [82], hybrid perovskite metasurfaces [Figs. 5(b) and 5(c)] [83], and all-dielectric metasurfaces used as an efficient ultra-broadband reflector [Fig. 5(d)] [84].
Another approach is the so-called UV NIL that employs a liquid-phase polymer spin-coated on a substrate. During the imprint step, the coated substrate is cured to form polymer crosslinking and generate solidified polymer by UV radiation. Therefore, the mold must be made of UV-transparent materials, and the process can be done with low imprint pressure at room temperature. Metasurface thermal emitters for infrared CO2 sensing are manufactured with UV NIL, followed by monolayer lift-off based on a soluble UV resist, shown in Fig. 5(e) [85]. Figure 5(f) reveals that a UV-NIL-fabricated metasurface has superior extinction in the unidirectional optical transmission mode from visible to infrared [86].
NIL holds the advantages of high resolution, large area fabrication and low cost. Parallel fabrication can be implemented with NIL for high yield and mass production as well. However, this method still requires a mold to be fabricated with high-resolution equipment. Furthermore, oxygen or argon-oxygen plasma etching is a necessary step to remove the residual imprint polymer layer during which the imprinted polymer may be degraded.
2.2.3 Self-assembly lithography
When it comes to large-area nanostructures, self-assembly lithography is an efficient and facile method. One of the promising self-assembly techniques is nanosphere lithography (NL). The NL technique combines the low cost of colloidal self-assembled polystyrene (PS) spheres as a hard mask with the subsequent etching or deposition process. This process of generating regularly-arrayed nanospheres is simple and cheaper as demonstrated in Fig. 6(a) [87]. A monolayer of PS spheres is self-assembled in a compactly arrayed hexagonal lattice at the interface between air and water. The monolayer is then transferred onto a target substrate by slowly withdrawing the water out of a container. Figure 6(b) shows a dielectric metasurface that functions as a near-perfect mirror on a silicon-on-insulator (SOI) substrate which is manufactured with a self-assembled monolayer of the PS spheres as a hard mask for etching [87]. It should be noted that the reflectivity of the silicon metasurface is less sensitive to the residual disorder and the asymmetry of the PS technique. This can be attributed to the fact that the silicon cylinders possess magnetic dipolar resonances rather than the electric resonances. All-dielectric metasurfaces can also be fabricated on a flexible substrate via the NL process for sensing applications [Figs. 6(c) and 6(d)] [88]. The flexible substrates are made of polyethylene terephthalate (PET), a polymer commonly used for bearing complex electronic systems, because of its optical transparency at visible wavelengths.
The conventional NL has so far been limited to producing simple periodic patterns. To open up new possibilities for creating more complex periodic nanostructures, other modified NL techniques have been developed. The shadow NL exploits sequential deposition from multiple angles with multiple plasma-etched colloidal masks to fabricate more complex structures [Figs. 6(e) and 6(f)] [89]. Engineered shadows of spheres provide a new strategy to efficiently prototype periodic metasurfaces. Besides, the moiré NL utilizes two stacked layers of PS nanospheres as the masks for etching and metal deposition to create metasurfaces with moiré patterns [Fig. 6(g)] [90] that feature high rotational symmetry and support multiple surface plasmon modes, leading to broadband field enhancement. NL lithography is an inexpensive technique that can be applied to large-scale substrates, but uniformity has been a significant challenge.
Laser-induced, self-organizing technique was proposed to fabricate large-scale resonant metasurfaces on Si thin films [Fig. 7(a)] [91]. The desired surface morphology of a Si thin film is obtained through deformation induced by the incident femtosecond laser pulses at a given wavelength. This is a self-adjusting approach that eliminates the need for multiple lithography steps by imprinting the interference pattern of the incident and scattered laser pulse directly onto the film. Figure 7(b) shows the metal particle array that is self-assembled by the block copolymer (BCP) on a thermal shrinkage film — a polymeric substrate [92]. The subsequent pattern shrinkage allows for period and symmetry control. Figure 7(c) shows a highly tunable refractive index metasurface constructed using the BCP self-assembly that operates in a broad wavelength range spanning across the visible region [92]. The Langmuir–Blodgett trough shown in Fig. 7(d) is a robust and scalable assembly method that can be used to construct a metasurface with close-packed Ag nano-cube arrays [93]. Such fabrication process can introduce colloidal nanocrystals of various shapes onto metasurfaces for different purposes. Figure 7(e) reveals the SEM image of the close-packed Ag nano-cube metasurface that exhibits near-ideal electromagnetic absorbance which can be tuned from visible to mid-infrared. The wrinkled template can support self-assembly as well. Assembly occurs once the wrinkled template is withdrawn from a container with a solution full of nanorods [94]. AFM image of a magnetic metasurface fabricated with the self-assembly process by dip-coating the wrinkled template in a highly concentrated Au nanorod solution is shown in Fig. 7(f) along with the schematic of the process.
2.3 Hybrid patterning lithography
Hybrid patterning techniques combining various aforementioned lithography methods are developed to realize metasurfaces with more complex nanostructures (Table 3). Two such methods are discussed here.
2.3.1 Micro-sphere projection lithography
Projection lithography offers new capabilities in rapid-prototyping of periodic and quasi-periodic metasurfaces. It uses self-assembled arrays of silica spheres as colloidal microlenses. Each microlens projects an image of a distant, macroscopic mask onto the coated substrate. Figure 8 (a) depicts the schematic of the fabrication process for aperiodic metasurfaces from the template in silicon to the final substrate [95]. The beads are selectively adhered inside the wells in the silicon wafer filled with polyethylenimine (PEI). The PEI is removed by thermal decomposition with a butane torch. The array of beads is picked up with a polymer slab and then placed in contact with the substrate. After the exposure and development, the pattern is transferred by metallization and lift-off or by etching [Fig. 8(b)] [95].
The method features size in the range of 0.4-10 μm and is suitable for academic research on metasurfaces. This is because efficient verification between theory and experiment requires generation of new designs rapidly over large areas and at low cost.
2.3.2 Hole-mask colloidal and off-normal deposition
Several challenges remain to realize directional metasurfaces with tilted nanopillars that are compact, scalable and cost-effective to produce in large quantities. Figure 8(c) combines an inexpensive and high throughput hole-mask colloidal lithography method, and off-normal deposition to fabricate the directional metasurfaces [96]. At first, the PS spheres are randomly dispersed on a substrate coated with polymethyl methacrylate (PMMA) followed by the deposition of a thin metal film. The hole-mask is formed by removing the PS spheres through the use of tape stripping. Tilted nanopillars are created after the deposition at an off-normal angle and the removal of PMMA.
Figure 8(d) shows the plasmonic metasurfaces with an out-of plane asymmetrical, aligned, and tilted subwavelength Au nanopillars [96]. These structures produce directional optical response as a result of light scattering off these asymmetrical structures.
2.4 Alternative techniques
While the three categories of fabrication techniques reviewed above have all played important roles in demonstrating optical metasurfaces and their unconventional applications, they each have certain limitations that leave space for innovation and improvement. As the community continues its search for innovative techniques, it is important to realize that some existing fabrication techniques could be but not yet applied to the making of optical metasurfaces. These methods offer great potential in expanding the versatility and functionality of metasurface in the near future (Table 4).
2.4.1 Laser-induced forward transfer lithography
Although the multi-exposure EBL technology has been used to fabricate multi-layer micro- and nanostructures, the method is rather complex to use because of the difficulty in alignment error in addition to being a time-consuming process. Laser-induced forward transfer (LIFT) is a versatile and high-throughput fabrication technique based on the LDW technology [Fig. 9(a)] [97,102]. The main idea behind LIFT is energy transformation where the pulsed laser beam passes through the supporting transparent substrate and gets focused on a donor material. The optical energy of the laser pulses is then transformed into the kinetic energy of the donor material. As a result, the illuminated material can be ablated forward and deposited on an opposite receiver substrate [Figs. 9(b) and 9(c)] [97,102].
The setup and operation of the LIFT experiment are fairly simple and low-cost since LIFT is a kind of LDW process. Most LIFT-correlated processes only require ambient atmospheric conditions without the demand of a clean room, chemical compounds and vacuum chambers. This simple, fast, and one-step technique shows great potential in micro- and nano-device fabrication.
2.4.2 Laser ablation and laser-induced dewetting
Laser ablation is another interesting technique where materials are lifted off from the surface of a substrate with a focusing laser. The removed quantity depends on the material as well as the wavelength, intensity and pulse width of the excitation laser. Dense hotspots in Ag nanostructures have been demonstrated with the laser ablation method [103]. The structure of recorded mark on a phase-change thin film under the laser ablation process has been reported as shown in Fig. 9(d) [98].
Dewetting of a heated material is one type of self-assembly process. Laser radiation as a heat source can launch the dewetting process. Laser-induced dewetting is a single-step, lithography-free and cost-efficient method for large-scale fabrication of ordered and disordered structures [Fig. 9(e)] [99]. The method opens up new possibilities for creating nanostructures in metal, dielectric, semiconductors and multilayer substrates on large-scale.
2.4.3 Two photon lithography
3D micro- and nanostructures have long been sought for but their fabrication has faced significant technical challenges. The lithography techniques have severe limitations here because of their high cost, prohibiting their applications to the fabrication of such complex structures [100,101,104–107]. Two-photon lithography with ultrashort laser pulses is an effective and well-established method in polymerization of arbitrary 3D structures. Polymerization occurs once a molecule is excited from one state to a higher energy state by absorbing two photons of identical or different frequencies [Figs. 9(f)-9(h)] [100,101]. The advantages of two-photon method are good geometry control, scalable resolution and cleanroom free. At the same time, the low efficiency of two-photon absorption and the limitation of photosensitive materials remain significant challenges.
3. Applications of metasurfaces
Novel optical metasurfaces that promise ultrathin, lightweight, and ultra-compact advantages over the bulky and heavy conventional optical devices have revolutionized the ways with which electromagnetic waves can be controlled and manipulated. A wide variety of functionalities that were impossible to realize in conventional devices are now made possible with optical metasurfaces. In this section, we shall survey some of the applications that have arisen from these novel devices over the last couple of years. In particular, we shall focus on those applications that rely on wavefront shaping, polarization control and active tuning.
3.1 Wavefront shaping
Wavefront engineering for conventional optical elements relies on the spatial refractive-index distribution, surface topography and phase accumulation along the optical path. Some examples are illustrated here to show how these purposes are realized such as beam splitting, beam steering, metalens, meta-hologram and optical vortex generation. Two of the hot topics in metasurface development have been the control of their strong phase dispersion and the ability to extend their working bandwidth. We shall review metasurfaces designed and fabricated for monochromatic and broadband operations. We shall also discuss wavelength dispersion in these devices.
Beam steering as a unique function of metasurface was first proposed and demonstrated by Capasso’s group in 2011 [4]. With the abrupt phase change at the surface, the new wavefront with anomalous propagation direction can be created by orderly arranging the nano-resonators on a metasurface. The anomalous propagation direction has been found to follow the generalized Snell’s law that takes into account of the index gradient along the in-plane direction of metasurface which can be tuned by design in order to achieve manipulation of wavefront. Recently this law has been applied to metasurface composed of supercells with various phase differences by Ho et al. [108]. Metalens is another application of the wavefront shaping. The phase retardation distribution of a metalens can be described as:
where λ is the wavelength in free space and f is the focal length. In order to avoid the high intrinsic loss that noble metal has in the visible range (400 to 700 nm), dielectric material has been used in these metalenses. Khorasaninejad et al. demonstrated visible-range diffraction-limited metalenses using titanium dioxide (TiO2) nanofins with Pancharatnam-Berry phase rotational morphology and have achieved efficiency as high as 86% [Figs. 10(a) and 10(b)] [109]. TiO2 nanofins are further used to construct a metalens with an engineered dispersive response that focuses incident light beams with opposite helicities into two distinct foci, demonstrating a chirality-distinguishable imaging system [Fig. 10(c)] [110]. Chen et al. proposed a pixel-level full-color routing device composed of GaN nanorods with off-axis focusing with visible light, showing a low-cost fabrication and high-efficiency platform for metalenses [Fig. 10(d)] [69].In addition to shaping of symmetrical wavefront, metasurfaces can be designed to generate arbitrary wavefront. In comparison to holograms created by conventional methods, optical metasurfaces can enhance the hologram imaging performance. The computer generated hologram (CGH) technique has been used to calculate the phase distribution requirement for holographic images. Meta-holograms have been demonstrated recently to show high contrast, multiplexing and tunability. Shown in Figs. 11(a) and 11(b), Kivshar’s group has realized grayscale meta-holograms composed of a set of 36 different high-index Si nano-pillars with a measured transmission efficiency up to 90% and diffraction efficiency over 99% at 1600 nm [111]. Our group has demonstrated a multi-color hologram utilizing Al nano-rods with different sizes to form a two-level phase modulation that is polarization- and wavelength-dependent. The hologram images are re-constructed at different angles for three primary colors [Fig. 11(c)] [112]. Wang et al. has proposed a metasurface consisting of three kinds of Si nano-blocks with subwavelength spacing and in-phase orientations in order to achieve full phase control in red, green, and blue [Fig. 11(d)] [113]. They have also demonstrated achromatic and highly dispersive meta-holograms by creating identical images at different wavelengths and distinct images at identical wavelength. To extend the practicability of meta-holograms, a reprogrammable 1-bit meta-hologram whose state can be switched between 0 and 1 by electrically controlling the loaded diodes is demonstrated by Li et al. [Fig. 11(e)] [114]. Malek et al. proposed a reconfigurable meta-hologram with Au nanorods on a stretchable polydimethylsiloxane substrate where the hologram image plane can be multiplexed by stretching [117].
Optical phase singularities have recently received much interest due to their various promising applications in nonlinear optics [118], quantum information technology [119], optical tweezers and so on. Vortex beam is typically created by fork diffraction gratings and spiral phase plates. Chen et al. demonstrated a novel type of geometric metasurface fork grating that seamlessly combines the functionality of a metasurface phase plate for vortex-beam generation and that of a linear phase gradient metasurface for controlling the wave-propagation direction [Figs. 11(f) and 11(g)] [115]. Qiu’s group proposed an ultrathin nanostructured optical vortex generator with multiple focal planes along the longitudinal direction by combining the functionalities of spiral phase plates and focusing lens [Fig. 11(h)] [116]. The polarization state and the position of the focal plane can be controlled by manipulating the helicity of the incident light. They designed a series of Pancharatnam-Berry phase metasurfaces to produce the perfect vortex and vector beams, replacing the conventional vortex plate, Bessel converter and lens.
Wavelength dispersion of optical materials is known to affect the performance of optical components and systems. To eliminate chromatic aberrations, the concept of achromatic metalens that imparts a wavelength-dependent phase contribution is proposed to compensate the dispersive accumulated phase through light propagation. Aieta et al. realized achromatic metalens using an aperiodic arrangement of coupled rectangular dielectric resonators, which operates at telecomm wavelengths [Fig. 12(a)] [120]. This design preserves the same focal length when the lens is illuminated with near-infrared light beams at three discrete wavelengths of 1300, 1550, and 1800 nm. Similarly, Faraon’s group presented a method for designing multi-wavelength metasurfaces using unit cells with meta-atoms of different resonant modes which can be used to implement a lens with two focal distances at two wavelengths, or a lens converging at one wavelength and diverging at the other [Fig. 12(b)] [121]. Avayu et al. introduced dense vertical stacking of independent metasurfaces, where each layer is made from a different material, and is optimally designed for a different spectral band [Fig. 12(c)] [122]. Khorasaninejad et al. proposed an achromatic metalens operating over a continuous 60-nm bandwidth in the visible [Fig. 12(d)], although the bandwidth is not enough for practical applications at the moment [123]. Our group proposed a design principle to realize achromatic metasurface that can eliminate the chromatic aberration over a continuous wavelength region from 1200 to 1680 nm for circularly-polarized incidence in a reflection scheme [Fig. 12(e)] [68]. Integrated unit elements on metasurface with smooth and linear phase dispersion are used to compensate the phase requirement of different wavelengths.
Contrary to the effort to eliminate wavelength dispersion, the use of dispersion of metasurface can also provide opportunities for applications that capitalize the effect. Arbabi et al. experimentally demonstrated dielectric gratings and focusing mirrors exhibiting positive, negative, zero, and enhanced dispersions [Fig. 12(f)] [124]. Super-dispersive off-axis metalenses for high resolution spectroscopy have also been demonstrated [125].
3.2 Polarization control
As a fundamental property of electromagnetic waves, polarization has been widely used in a wide range of applications. Conventional optical components usually rely on the birefringence of crystals to manipulate the polarization states of light. Orthogonally polarized waves propagating through the crystal accumulate different phases between two principal axes. These optical components suffer from a number of drawbacks such as being bulky and heavy with narrow operating bandwidth and limited material choices. Metasurface-based wave plates being light and compact, on the other hand, promise to be capable of broadband operation with a range of materials to choose from. Such wave plates can modulate the phase delay between two orthogonal polarizations by splitting the incident light. We shall review the recent development of metasurface-based wave plates for applications ranging from low-phase modulation in quarter-wave plates to high-phase modulation in polarimetry.
Although metasurfaces consisting of nano-antennas made of noble metal were initially used to demonstrate quarter-wave plates, dielectric metasurfaces have been introduced to improve device efficiency in visible and near-infrared range. Recently transparent conducting oxides (TCOs) developed as part of the CMOS-compatible process are being investigated as alternative materials for dielectric metasurfaces. Kim et al. fabricated a TCO metasurface working as a quarter-wave plate in the reflection mode as shown in Figs. 13(a) and 13(b) [126]. The metasurface can be operated over the broad bandwidth in the near-infrared regime (λ = 1.75 to 2.5 μm). The reflected beam exhibits a high degree of circular polarization state close to unity [Fig. 13(c)].
Circular dichroism (CD) is a phenomenon that takes place when the left-circularly polarized (LCP) and the right-circularly polarized (RCP) components of the incident light experience different transmittance. Hu et al. developed an all-dielectric metasurface composed of Z-shaped chiral structures of silicon film on a SiO2 substrate to realize the CD waveplate in the transmission mode [Figs. 13(d) and 13(e)] [127]. Experimental results show CD up to 97% and a high extinction ratio of 345:1. Polar diagrams for the polarization state of the metasurface-based CD waveplate clearly show that the RCP incident component is being transmitted while LCP reflected [Figs. 13(f) and 13(g)]. To demonstrate continuous linear-to-circular dynamic control of the polarization state, Liang et al. developed a monolithically integrated metasurface structure where metallic antennas are integrated onto a SPP waveguide [Figs. 13(h) and 13(i)] [128]. The SPP waveguide couples radiation from a semiconductor-based THz quantum cascade laser (QCL) into SPP waves which are then scattered and collimated into the direction that is perpendicular to the waveguide surface. The emitted laser beam with desired polarization can then be generated with the careful design of the metasurface. When the emitted intensities of the two laser beams with π/2 phase difference are manipulated independently, the polarization state of the combined beam can evolve continuously from linear to circular [Figs. 13(j) and 13(k)].
Metasurface-based half-wave plates appear to be more difficult to produce because the phase difference up to π needs to be sustained between the two orthogonal polarizations with equal amplitudes. Liu et al. proposed a generic method to design the half-wave plate that is wavelength independent based on the Pancharatnam-Berry geometric phase and the mirror effect of anisotropic optical antennas [Figs. 14(a) and 14(b)] [129]. The bisection angle of the antenna pairs determines the optics axis where the incident and image polarizations have mirror symmetry. Experimental results in Fig. 14(c) show high degree of linear polarization in the transmitted image in the near-infrared range.
Wu et al. fabricated a bi-layer ultrathin anisotropic metasurface as a half-wave plate to convert the circularly polarized light almost completely to its cross polarization [Fig. 14(d)] [130]. The metasurface is composed of an F4B substrate on which either side is deposited with periodic 180°-twisted double-cut split ring resonators. Simulation and experiment demonstrate that the transmission efficiency of cross-polarized light is greater than 94% at the resonant frequency in microwave regime [Figs. 14(e) and 14(f)]. The resonance frequency can be effectively adjusted by changing the geometric parameters of the metasurface. Park et al. further presented an actively controllable metasurface that operated in a reflection scheme [Fig. 14(g)] [131]. Figure 14(h) demonstrates that the largest swing in the reflection phase reached over 180° with the electrical tuning of the gap-plasmon resonators featuring the metal-insulator-metal (MIM) structure near critical coupling. However, such high swing in the reflection phase is accompanied with substantial loss.
The ability to extract useful information from light polarization has motivated the invention of polarimetry. This optical component is developed to determine the polarization state and Stokes parameters of an arbitrary light source. Our group has numerically and experimentally displayed a reflective metasurface polarization generator (MPG) to simultaneously produce six polarization states from a single light source with linear polarization [Figs. 15(a) and 15(b)] [132,134]. The MPG composed of gap-plasmon resonators is capable of broadband operation in the visible regime since Al is chosen as the plasmonic metal and the concept of design is based on the Pancharatnam-Berry theory. The efficiency variation at different locations of the proposed MPG remains small. High broadband extinction ratios for all generated polarization states in the visible regime have been achieved as shown in Fig. 15(c).
The orbital angular momentum (OAM) of light is the component of angular momentum of a light beam that is dependent on the field spatial distribution but not on polarization. It has drawn much attention due to its versatile applications arising from superposition of OAM states, such as vector beam generation, ultrasensitive angular measurement, spin object detection, quantum entanglements, and so on. Yue et al. has employed the Pancharatnam-Berry geometric phase to experimentally validate a single broadband gap-plasmon metasurface capable of generating superposition of multiple OAM states [Fig. 15(d)] [133]. The polarization of incident light can be simply tuned to create arbitrary superposition of OAM states in four channels as shown in Figs. 15(e)-15(g). This method has diverse applications in both classical and quantum physics.
3.3 Active metasurfaces
A major challenge to develop a multi-functional optical component is to decouple the strong correlation between its physical geometry and optical functionality. Putting together several optical elements of different functions is one way to solve the problem. But this solution inevitably encounters other undesirable challenges such as complex fabrication processes, overly sophisticated surface morphology, and bulky devices. Even when they are successfully made, multi-functional metasurfaces created this way lack the ability to actively manipulate their optical responses. There is obviously a need to develop actively tunable metasurfaces to replace the static multi-functional optical components. In this section, we shall survey tunable metasurfaces that are controlled with either mechanics, electricity, temperature or light.
Gutruf et al. demonstrated a mechanically tunable all-dielectric resonator metasurface at visible frequencies as shown in Fig. 16(a) [135]. This metasurface is composed of an array of dielectric resonators embedded in a flexible substrate made of PDMS that can be mechanically bended and stretched. The optical response of the metasurface exhibits remarkable resonance shifts under different degrees of uniaxial strain. As shown in Figs. 16(b) and 16(c), Ee et al. demonstrated a mechanically reconfigurable metasurface capable of continuous manipulation of light wavefront by changing the lattice constant of an embedded Au nanorod array through stretching the substrate [136]. These efforts have paved the way for the development of reconfigurable broadband optical devices.
Being able to electrically control the functionality of a metasurface is always desirable for fast switching and ease of operation. Buchnev et al. proposed a scheme with which an active near-infrared metasurface loaded with nematic liquid crystal (LC) can be electrically controlled to shift its resonance in near infrared [Figs. 16(d)-16(f)] [137]. As a well-established and affordable technology, LCs in the nematic phase offer interesting material properties such as broadband optical non-linearity and birefringence. However, the strong anchoring force from the interaction of nematic LC molecules with the surface limits the efficiency of the LC-loaded devices. In order to circumvent this issue, a suspended metasurface was fabricated, successfully eliminating the strong surface anchoring effect of LC molecules by reducing the area of the supporting substrate as shown in purple [Fig. 16(d)]. This work opens up metasurface-based applications in light modulator, switches, or active control in beam steering and polarization.
Hashemi et al. demonstrated active beam steering with an electronically-controlled metasurface made of vanadium dioxide (VO2) [Fig. 16(g)] [138] which is a phase-change material that behaves like a semiconductor at room temperature and enters an abrupt insulator-to-metal transition that is triggered by either thermal, electrical, optical or mechanical stimulation. Steering is achieved by controlling the electric current applied to individual unit-cells and collectively they shape up the wavefront of the transmitted electromagnetic wave and deflect it to specified directions. Wang et al. also used VO2 to realize metasurface-based switchable quarter-wave plate in terahertz [140]. Such metasurface is composed of complementary electric split-resonators embedded in VO2. Moreover, Dabidian et al. experimentally demonstrated electrical control of the reflectivity in mid-infrared using back-gated single layer graphene (SLG) as shown in Figs. 16(h) and 16(i) [139]. SLG is a promising 2D material for light modulation because electrostatic or chemical doping can alter its optical conductivity. Efficiency in modulating mid-infrared reflectivity can be improved by integrating plasmonic metasurfaces with SLG. An order of magnitude improvement has been demonstrated with this approach.
Instead of electrical control, Sautter et al. developed an all-dielectric metasurface with a nematic LC cell that can be tuned with heat to dynamically adjust electric and magnetic resonances in near infrared [Figs. 17(a) and 17(b)] [141]. As shown in Fig. 17(c), with the increase of the nematic LC temperature, a dramatic spectral shift in the electric resonance is appeared from the embedded metasurface while the spectral position of the magnetic resonance remains unchanged below the phase transition temperature of about 58 °C.
To demonstrate active metasurfaces controlled with light, Wang et al. exploited light-induced phase transition of germanium antimony telluride (GST) alloy to accomplish a variety of metasurface-based devices such as Fresnel zone plate, lens and hologram [Fig. 17(d)] [142]. The GST alloy is another important phase-change material with advantages of low optical loss in near-infrared, non-volatility, high stability, and quick response. The material can be melted or quickly quenched to an amorphous state with a short high-density laser pulse and transformed back into a metastable cubic crystalline state at an annealing temperature between the glass transition and the melting point. The use of GST rod as a basic building block for all-dielectric metasurfaces was numerically simulated [144]. Furthermore, the GST nano-grating metasurface was experimentally demonstrated for high-quality near-infrared transmission and reflection resonances as shown in Fig. 17(e) [143].
4. Conclusions
In less than a decade since the inception of metasurface, a wide range of fabrication technologies have been developed and applied to demonstrate some of the amazing features that conventional optical elements cannot produce. Still, the pursuit of more advanced fabrication methods and perfection of existing techniques are ongoing in order to meet the demands for low cost, high throughput, large area, good reproducibility, and high resolution. In this paper, numerous fabrication techniques of the optical metasurfaces with static and tunable functions have been surveyed. The maturity of these fabrication techniques along with the development of novel materials is the key to the future of optical metasurfaces. Wavefront shaping and polarization control using metasurfaces have seen impressive progress in recent years. Active metasurfaces with tunable functionality continue to emerge. A number of applications of the optical metasurfaces are not included in this article, such as nonlinear metasurfaces [145–151], parity-time symmetry metasurfaces [152–154], and so on. Effort in the community is picking up at an accelerated pace for more advanced optical metasurfaces that will revolutionize the optics industry in the not-so-distant future and change the way people think about what the ultrathin optics can do.
Funding
The authors acknowledge financial support from Ministry of Science and Technology, Taiwan (Grant No. MOST-106-2745-M-002-003-ASP) and Academia Sinica (Grant No. AS-103-TP-A06). Authors are also grateful to National Center for Theoretical Sciences, NEMS Research Center of National Taiwan University, National Center for High-Performance Computing, Taiwan, and Research Center for Applied Sciences, Academia Sinica, Taiwan for their supports. G. S. acknowledges support from Air Force Office of Scientific Research (Grant No. FA9550-17-1-0354).
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