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Metalenses: Advances and Applications

Ming Lun Tseng, Hui-Hsin Hsiao, Cheng Hung Chu, Mu Ku Chen, Greg Sun, Ai-Qun Liu, and Din Ping Tsai*

DOI: 10.1002/adom.201800554

and optoelectronics. Metasurfaces as 2D artificial photonic structures are com-posed of subwavelength resonators (often referred to as meta-atoms).[1–8] The optical responses/functionalities of metasurfaces can be tailored by choosing the proper geometrical parameters of these meta-atoms.[9–14] They have been applied to realize ultrathin invisible cloaking,[15] metahologram,[16–20] surface plasmon launchers,[21–23] compact nonlinear devices,[24–28] nanolasers,[29–34] and many novel compact photonic devices.[11,35–57] Among all the promising applications of metasurfaces, planar metalenses with superior performance and functionalities over their conventional counterparts are definitely one of the most exciting and important research areas. This is because metasurface lenses (metalenses) can not

only show better optical functionalities but also allow for much more compact device design than the conventional high-end objective lenses. In this article, we will review the progress in the development of metalenses. This article is organized into three major parts. First, the working mechanisms of chromatic and achromatic metalenses will be introduced. The design principle of integrated-resonant units for correcting chromatic aberration of a metalens will be discussed. Second, novel appli-cations of metalenses mentioned in the first part for full color imaging, sensing, and spectroscopy will be reviewed. After the discussion of the passive metalenses, the emerging tunable metalenses and their applications will be surveyed, followed by concluding remarks on future prospects.

2. The Origin of Chromatic Aberration

Conventional refractive lenses rely on gradual phase accumu-lation along the optical path traveled by a light beam. This is accomplished either by controlling the surface topography or by varying the spatial profile of the refractive index. The chro-matic aberration in refractive optical components arises from material dispersion. In a material with normal dispersion, the refractive index decreases with increasing wavelength so that a refractive lens made of the same material has larger focal length in red than in blue. Diffractive optical devices, on the other hand, operate as the interference of light through an amplitude or phase mask. The deflection angle of a diffrac-tive grating varies with wavelength, where the rate of change depends on the pitch of the grating. Such dispersion is opposite

Metasurfaces, the 2D counterpart of artificial metamaterials, have attracted much attention because of their exceptional ability to manipulate the electro-magnetic wave such as amplitude, phase, polarization, propagation direc-tion, and so on. Different from conventional lenses, metalenses based on the metasurface optics are truly flat and compact and exhibit superior perfor-mance. In this report, recent progress in the development of metalenses is explored. First, the working principle and characteristics of metalenses are discussed. Then, it is described how the dispersion aberration in metalenses can be eliminated to make them suitable for being employed in a range of applications that are difficult or impossible for traditional lenses. In addition, various metalens-based applications are introduced, including imaging, high spectral resolution spectroscopy, and multiplex color routing. Furthermore, a survey of reconfigurable and tunable metalenses is conducted. Finally, the report concludes by addressing future prospects of metalenses.

Dr. M. L. Tseng, Dr. C. H. Chu, M. K. Chen, Prof. D. P. TsaiResearch Center for Applied SciencesAcademia SinicaTaipei 11529, TaiwanE-mail: [email protected], [email protected]. M. L. Tseng, Dr. C. H. Chu, M. K. Chen, Prof. D. P. TsaiDepartment of PhysicsNational Taiwan UniversityTaipei 10617, TaiwanProf. H.-H. HsiaoInstitute of Electro-Optical Science and TechnologyNational Taiwan Normal UniversityTaipei 11677, TaiwanProf. H.-H. HsiaoGraduate Institute of Biomedical OptomechatronicsTaipei Medical UniversityTaipei 11031, TaiwanProf. G. SunDepartment of EngineeringUniversity of Massachusetts at BostonBoston, MA 02125, USAProf. A.-Q. LiuSchool of Electrical and Electronic EngineeringNanyang Technological UniversitySingapore 639798, Singapore

The ORCID identification number(s) for the author(s) of this article can be found under https://doi.org/10.1002/adom.201800554.

Metalenses

1. Introduction

In recent years, optical metasurfaces have attracted much attention due to their great potential to advance photonics

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to the standard refractive optical elements (known as “nega-tive dispersion”),[58] where longer focal length corresponds to a shorter wavelength. In order to eliminate chromatic aberration, early effort has endeavored to achieve refractive or diffractive achromatic lenses by integrating or cascading them in the form of doublets and triplets to obtain the same focal length for mul-tiple wavelengths of interest. However, the composite configu-ration makes the optical system bulky, complicated, and costly.

Metasurfaces are thin optical elements comprised of spatially varying optical resonators with subwavelength separations that provide an entirely new mechanism for light control. In order to convert incident planar wavefront into a spherical one, one should impose the following phase profile[59]

ϕ λ ϕ λ πλ ( )− = = = − + + −x y x y x y f f( , , ) ( 0, 0, )

2 2 2 2 (1)

where x and y are the spatial coordinates with respect to the center of lens (x = y = 0), and f is the focal length of the designed lens. Since the required phase profile has a depend-ence on wavelength, a metalens must exhibit independent phase control at each desired wavelength to achieve achromatic focusing. However, if the desired phase coverage of 0−2π for metasurface-based devices can only be obtained by either var-ying the geometric dimensions of one set of meta-atoms or by rotating their orientations, the outcome is that this one set of meta-atoms can only satisfy the required phase for a given wavelength but not at other wavelengths which leads to chro-matic aberration. This causes the demonstrated devices in early times suffer from strong chromatic aberration even though metasurface-based optical elements can be designed to operate over a broadband wavelength range. The dependence of the deflection angle or focal length on wavelength significantly compromises their performance in full-color optical applica-tions such as imaging and displaying.

3. Metalens: Control of Chromatic Dispersion

3.1. Multiwavelength Achromatic Metalenses

Up to now much effort has focused on multiwavelength metade-vices aimed at improving the lens behavior at a discrete set of wavelengths.[60–63] Cappasso and co-workers utilized an aperi-odic arrangement of coupled rectangular dielectric resonators to provide the phase coverage at three wavelengths (Figure 1a). This design allows the incident near-infrared light to have the same focal length at λ = 1300, 1550, and 1800 nm with meas-ured efficiencies of 15%, 10%, and 21%, respectively.[64]

Composite metalenses in cascading or spatially multiplexing configurations have also been demonstrated, comprising of several sublenses with each one designed to fulfill the required phase profile at a specific working wavelength. Avayu et al. used a vertical stacking of three layers to demonstrate a triply red (650 nm), green (550 nm), and blue (450 nm) achromatic metalens (Figure 1b). Each layer consists of disc-shaped nano-particles made of different materials (aluminum, silver, and gold), and the parameters of the nanodiscs are optimized to support localized surface plasmon resonances for a specific

frequency band.[65] Arbabi et al. utilized spatially multiplexing high contrast dielectric metaslenses to achieve light focusing at wavelengths of 915 and 1550 nm to the same focal plane (Figure 1c). Two metalenses comprised of amorphous silicon (a-Si) nanoposts are designed for the operation at two different wavelengths and are combined via either large scale segmenta-tion or meta-atom interleaving arrangement.[66] Since the cou-pling among the nanoposts is relatively weak because each of

Greg Sun received his Ph.D. in Electrical Engineering from Johns Hopkins University, Baltimore, USA in 1993. He is now professor in engi-neering and physics at the University of Massachusetts Boston where he also serves as the founding chair of the Engineering Department. His research interests are in sem-iconductor optoelectronics,

silicon photonics, and nanophotonics. He is an associate editor for the Journal of Lightwave Technology.

Ai-Qun Liu received his Ph.D. degree in Applied Mechanics from National University of Singapore (NUS) in 1994. Currently, he is a pro-fessor at School of Electrical & Electronic Engineering, Nanyang Technological University (NTU). He serves as an editor and editorial board member of several jour-nals. Prof. Liu is interested in

the research fields of MEMS, nanophotonics, optofluidics, nano/microfluidics, and sensors for water and environ-mental monitoring. He is the author of over 160 publica-tions including peer-reviewed journal papers and two books. Also, he is OSA Fellow, RCS Fellow, and SPIE Fellow.

Din Ping Tsai received his Ph.D. degree in Physics from University of Cincinnati, USA in 1990. He is the Director and Distinguished Research Fellow of Research Center for Applied Sciences, Academia Sinica since 2012. He is also the Distinguished Professor of Department of Physics at National Taiwan University. He is a fellow of AAAS, APS, IEEE,

OSA, SPIE, and EMA. His current research interests are nanophotonics, near-field optics, plasmonics, metamaterials, green photonics, quantum photonics, and their applications.





them behaves like a multimode truncated waveguide, a unit cell consisting of multiple meta-atoms has more parameters to independently control the phases at different wavelengths. Thus, a unit cell with four different nanoposts was also utilized to effectively sample the desired phase profiles simultaneously at two wavelengths, achieving focusing efficiencies of 22% and 65% at 915 and 1550 nm, respectively, for NA = 0.46.[67]

Lin et al. used interleaved Si-based metasurfaces to eliminate the chromatic aberration at three primary colors: red, green, and blue wavelengths (480, 550, and 620 nm) (Figure 1d). Three metalenses were designed individually to focus light of these three colors at the same focal spot. They were then divided into a set of small segments randomly distributed across the whole area of the composite metasurfaces.[68] In


Figure 1. Multiwavelength achromatic metalenses. a) Metasurfaces consisting of coupled rectangular a-Si resonators focus three wavelengths of 1300, 1550, and 1800 nm to the same line. b) A vertical stacking metalens made of three different metallic nanodiscs shows the same focal distance at red (650 nm), green (550 nm), and blue (450 nm). c) Polarization insensitive metalenses comprised of a-Si nanoposts in large scale segmentation (upper panel) and interleaving arrangement (lower panel). d) A composite metalens comprised of three randomly segmented Si-based sublenses achieves light focusing at three primary red, green, and blue wavelengths to the same focal length. e) Double-wavelength metalens designed with birefringent elliptical meta-atoms.[69] f) Multispectral metasurfaces based on the spin–orbit interaction in elliptic nanoapertures. (a) Reproduced with permission.[64] Copyright 2015, American Chemical Society. (b) Reproduced with permission.[65] Copyright 2017, Nature Publishing Group. (c) Reproduced with per-mission.[66] Copyright 2016, Nature Publishing Group. (d) Reproduced with permission.[68] Copyright 2016, American Chemical Society. (e) Reproduced with permission.[69] Copyright 2016, Optical Society of America. (f) Reproduced with permission. Copyright 2015, Nature Publishing Group.[70]




addition, birefringent elliptical nanoposts were used to inde-pendently control the phases of two orthogonal polarizations at two different wavelengths (Figure 1e). With this approach the focal spots of the metalens at 780 and 915 nm under y- and x-polarized, respectively, appeared at the same position.[69] The measured efficiencies reach above 65% for all demonstrations with different NA values (up to 0.7) at both wavelengths. Zhao et al. demonstrated multispectral metasurfaces based on the spin–orbit interaction in elliptic nanoapertures to encode the phase information of many different wavelengths into a single metasurface (Figure 1f). The designed metalens exhibited unvaried focal length at wavelengths of 532, 632.8, and 785 nm, respectively.[70]

The design principles of these multiwavelength metal-enses mostly rely on the integration of several metalenses working at different targeted wavelengths into a single device. With the proper selection of constituent materials and careful design of meta-atoms, multiwavelength achromatic metalenses can be realized in near-IR and visible regime. This approach can be effective for applications that only need a few discrete operating wavelengths, such as in florescence microscopy and optical communication. However, with the increase of number (or bandwidth) of the working wavelengths, the design complexity goes up dramatically. At the same time, the unin-tended coupling and interference between metalenses become unavoidable. These undesirable effects will ultimately limit their effectiveness in certain applications such as white-light imaging and spectroscopy. A novel approach for the develop-ment of broadband achromatic metalenses is critically needed.

3.2. Continuous Broadband Achromatic Metalenses

The recent development in dispersion-engineered metasurfaces has led to the achievement of achromatic focusing over a con-tinuous broadband. Several works have been demonstrated in reflective mode to take advantages of the large reflection ampli-tude and overall increase of the phase coverage of metallic reflectors. Khorasaninejad et al. experimentally demonstrated an achromatic metalens made of titanium dioxide (TiO2) nanopillars and a metallic mirror separated by a dielectric spacer layer that exhibited a constant focal length over the contin-uous 60 nm bandwidth from λ = 490 to 550 nm (Figure 2a).[71] According to the calculated phase response of the nanopillars with different widths at a specific wavelength, they found that several choices of widths can achieve the same phase at the wavelength of interest and provide different dispersive values simultaneously. In addition, according to Equation (1), since the phase at the referenced lens center can have distinct values for different wavelengths, they used it as a free parameter in the optimization of the metasurface that minimizes the difference between the designed and implemented phase simultaneously for all selected wavelengths. Using the same approach, they also designed a metalens with a reverse chromatic dispersion where the focal length increases with increasing wavelength.

Arbabi et al. utilized a reflective metasurface composed of dielectric nanoposts to demonstrate versatile focusing effect with positive, zero, and hypernegative dispersions (Figure 2b).[58] Amorphous-Si nanoposts fabricated on a silicon

dioxide (SiO2) spacer above an aluminum reflector were used to simultaneously control the imparted phase and its wavelength derivative (phase dispersion). The zero dispersion metalens exhibits a highly diminished chromatic dispersion in the wavelength range of 1450–1590 nm and maintains efficiency around 50% in the whole working spectra. On the other hand, the hyperpositive and hypernegative dispersion metalenses have a dispersion that is twice and 3 1/2 times, respectively, larger than a regular negative one.

Recently, Tsai and co-workers proposed the use of integrated-resonant units (IRUs) in metasurfaces to realize smooth and linear phase dispersion in combination with geometric phase for the design of reflective achromatic metalenses capable of operating in broad infrared bandwidth of 1200–1680 nm (Figure 2c).[72] The design utilized a sandwich structure formed by a couple of specially arranged gold (Au) nanorods, SiO2 spacer, and Au back reflector as the basic IRU building block. With careful design of the multiple resonances of the nanorods, the phase dispersion of IRUs can be manipulated to achieve different phase-changing slopes. Larger phase com-pensation can be directly realized by adding more resonators into the unit cells. In addition, the phase value at the refer-enced lens center is defined as ϕshift(λ) = p/λ + q to adjust the required phase compensation profile so that the phase disper-sion of designed IRU building blocks can appropriately satisfy the required phase profile at each sampling positions, where

λ λλ λ

=−

p max min

max min

and λ

λ λ= −Ψ

−q min

max min

, and Ψ denotes the largest

additional phase shift between λmin and λmax at the central position of the metalens. A similar strategy was applied to alu-minum (Al) sandwich structures to construct achromatic met-alenses capable of operating in visible (Figure 2d).[73] As Al has higher plasma frequency than Au, their reduced absorption in visible leads to better performance in efficiency compared with Au. The demonstrated Al metalenses show unvaried focal dis-tance from 400 to 667 nm with efficiency above 20% over the working bandwidth.

While these reflective metalenses are truly innovative in demonstrating broadband achromaticity, transmissive optical components are much more attractive and highly desirable for many practical applications. Tsai and co-workers have recently utilized GaN-based IRUs to achieve an achromatic metalens operating in the entire visible region in transmission mode (Figure 3a).[74] Compared to the metallic IRUs that utilize near-field coupling between the resonators to achieve phase disper-sion modulation, the optical coupling of dielectric nanopillars is relatively weak, but the high-index dielectric resonator can be functionalized as a truncated waveguide supporting multiple Fabry–Pérot resonances. Tsai and co-workers therefore used high-aspect ratio GaN nanopillars and complementary struc-tures made of nanohole arrays drilled in a GaN film to accom-plish large phase compensation. The resulting metalenses demonstrated unvaried focal length from 400 to 660 nm with 40% average efficiency. In addition, Chen et al. utilized two TiO2 nanofins in close proximity as coupled waveguides with Pancharatnam–Berry phase method to independently tailor the phase, group delay, and group delay dispersion of metalenses (Figure 3b). They achieved achromatic imaging from 470 to 670 nm with efficiency of about 20% at 500 nm.[75]





Three different meta-atoms have been proposed so far to achieve broadband achromatic metalenses, namely, metallic nanorods (Figure 4a), dielectric nanoposts (Figure 4b), and complementary dielectric resonators (Figure 4c). Using metallic meta-atoms, the resonance layer can be made very thin (typically less than 100 nm). Metalenses can work in vis-ible with the use of aluminum as the constituent material. However, the intrinsic loss of these metallic meta-atoms and

the need for the back-reflection layer restrict this type of metal-enses to applications.

In the approach of coupled dielectric nanoposts, meta-atoms of high refractive-index and low-loss dielectric materials such as TiO2 and GaN can have strong optical resonances with near-zero optical loss. In addition, metalenses composed of dielectric materials can work in the transmissive mode. However, the coupling between dielectric nanoresonators


Figure 2. Reflective achromatic metalenses operating in continuous broadband. a) Building blocks made of TiO2 nanopillars, a dielectric spacer, and a metallic back reflector were applied to realize an achromatic metalens with over 60 nm continuous bandwidth achromaticity.[71] b) Dispersion-engi-neered metasurfaces with positive, zero, and hypernegative dispersions.[58] c) Au-IRUs metalens displaying unvaried focal distance in a broad infrared bandwidth of 1200–1680 nm.[72] d) Visible Al-IRUs metalens achieving achromatic focusing from 400 to 667 nm.[73] (a) Reproduced with permission.[71] Copyright 2017, American Chemical Society. (b) Reproduced with permission.[58] Copyright 2017, Optical Society of America. (c) Reproduced with permission.[72] Copyright 2017, Nature Publishing Group. (d) Reproduced with permission.[73] Copyright 2018, Wiley-VCH.




is typically a weak process, making it difficult to effectively manipulate the phase dispersion and maintain high efficiency simultaneously. The complementary dielectric resonant units, on the other hand, can be employed to overcome such a difficulty. Their optical resonances are associated with the high-order waveguide-like resonances inside the meta-atoms and their phase dispersion can be tailored by modifying the geometrical parameters of the meta-atoms, allowing for easier attainment of the desired phase dispersion. As a result, one can have the freedom to choose an optimized set of meta-atoms to realize a high-efficiency metalens. Moreover, besides chromatic aberration, other aberrations, such as monochro-matic,[76] coma,[77] astigmatism,[78] can be resolved by using metalenses as well. The state-of-the-art achievements on

achromatic metalenses aresummarized in Figure 5. Achro-matic metalenses with continuous working bandwidth are connected by solid lines indicating their working spectral range, while achromatic metalenses with discrete working wavelengths are marked by various symbols at the achromatic wavelengths connected by dashed line. The square and tri-angle symbols indicate the operation in either transmissive or reflective mode, respectively. In summary, two approaches have been reported to realize achromatic metalenses. In the first approach, multiple metalenses are integrated together. Due to the compact nature of metalenses, the integrated devices are still much thinner than the conventional lenses. The second approach is to introduce various meta-atoms with well-designed dispersion curves. As a result, the phase profiles


Figure 3. Broadband achromatic metalenses in transmission mode. Metalenses a) made of GaN nanopillars and nanoholes to demonstrate a con-stant focal length over from 400 to 660 nm,[74] and b) made of coupled TiO2 nanofins to achieve achromatic imaging from 470 to 670 nm. Scale bars: 500 nm. (a) Reproduced with permission.[74] Copyright 2018, Nature Publishing Group. (b) Reproduced with permission.[75] Copyright 2018, Nature Publishing Group.

Figure 4. Approaches to design a broadband achromatic metalens. Three kinds of meta-atoms have been used to design an achromatic metalens. a) Coupled metallic nanorods.[73] The electric field distribution associated to the coupling of three Al nanorods can be observed. b) A schematic of the resonant mode between two coupled dielectric nanoposts.[79] c) Simulated magnetic energy distribution on complementary dielectric resonan-tors.[74] (b) Reproduced with permission.[79] Copyright 2018, Nature Publishing Group. (c) Reproduced with permission.[74] Copyright 2018, Nature Publishing Group.




of the metalens at different working wavelengths can be pre-cisely tailored. Although the device design is more challenging in the second approach, it has several advantages in terms of device size and fabrication cost.

4. Applications of Metalens

As a planar optical device, metalens has the advantage for being ultrathin, lightweight, and ultracompact. A wide variety of functionalities that are impossible to realize in conventional devices are now made possible with optical metalenses. In the following, we shall discuss the applications of metalenses, including imaging, chiral sensing, hyper spectroscopy, as well as color routing. Perspectives on future directions of the met-alens technology will also be discussed here.

4.1. Imaging

Human beings arguably obtain most information from the outside world through our eyes—an unartificial imaging/optical system perfected through milions of years of evolu-tion to develop the ability to focus and project colorful image on retina. Metalens, a very recent technological advancement, is an artificial optical system that realizes the focusing ability by using various designs and materials. Constructing high-quality images with this system has proven to be a challenge owing to its low working efficiency in the visible region because of the intrinsic absorption in metals that are often used in the metalenses. Although reflection mode operation has achieved efficiency over 80%,[18] the architecture and operation of reflec-tive components in general tend to increase the complexity of the imaging system. Recently, this obstacle has been circum-vented by replacing metals with high index dielectric materials, such as titanium oxide (TiO2)[80] and gallium nitride (GaN).[81]

Chen et al. demonstrated a high-aspect-ratio titanium dioxide (TiO2) metalens with NA of 0.8[80] capable of achieving diffrac-tion-limited focal spots at the design wavelengths of 405, 532, and 660 nm where the highest efficiency can be as high as 86% (Figure 6a,b). High resolution and imaging qualities were also achieved.[80] Unfortunately, this metalens showed chromatic aberration that was resulted from the phase profile changes at different wavelengthes. Recently, Wang et al. developed an achromatic metalens composed of GaN meta-atoms that works for the entire visible region in transmission mode.[81] As shown in Figure 6c, the chromatic aberration correction was demon-strated in the wavelength region from 400 to 660 nm, exhib-iting about 49% bandwidth to the central working wavelength. Results clearly show that the achromatic metalens can resolve features separated by microscaled distances without chromatic aberration. Full-color imaging pictures (Figure 6d) were gener-ated from the broadband achromatic metalens—an important milestone in the development of metasurfaces for metalens-based full-color imaging.

4.2. Spectroscopy

As described above in Section 1, while the wavelength dis-persion of metalens often times has a negative impact to its performance in optical systems, the dispersion can in some applications be employed to improve specific optical systems when carefully designed. In a conventional spectrometer, in order to enhance spectral resolution, the distance between the grating and the detector needs to be large, which makes high resolution spectrometers particularly bulky. Chen et al. pro-posed an off-axis metalens (Figure 6e,f) as a hybrid component that combines the functions of focusing and dispersing at dif-ferent wavelengths with high spectral resolution in a compact configuration.[82] Silicon nanofins were used as building blocks and the phase requirement was satisfied by rotating the TiO2


Figure 5. State-of-the-art achromatic metalenses. The last name of the first author, adopted material for meta-atoms, and the publication year are listed.




meta-atoms. Taking advantage of the dispersion behavior of the metalens, the focal-line shifting with different wavelengths can be utilized to resolve the incident wavelengths with high pre-cision. The spectral resolution increases with focusing angle. When the focusing angle is set at 80°, a high dispersive char-acteristic of 0.27 nm mrad−1 can be obtained in the telecom region. The operating efficiency can be as high as 90% in the region of 1.1–1.6 µm. Furthermore, the working bandwidth can be extended by integrating several metalenses on a single chip. With the validation of high spectral resolution, the super-dis-persive off-axis metalenses exhibit good feasibility for compact and portable optical applications.

4.3. Full-Color Routing

As a demosntration of its practicality in device miniaturiza-tion, Chen et al. proposed a concept to integrate a metalens in a complementary metal-oxide-semiconductor (CMOS) sensor (Figure 6g).[83] The reported GaN-based dielectric metalens can function as a color router to guide three primary colors into different spatial positions. To seperate different colors in free space, the equal optical path principle is adopted to design the various phase profiles for different colors. As a result, the three primary colors at 430, 532, and 633 nm can be focused to arbitrary positions. Different from the super-dispersive off-axis

metalenses, the multiplex color router offers more degrees of freedom to focus different wavelengths to arbitrary positions individually. Furthermore, the GaN-based metalens reveals high operation efficiency in the visible region where the efficiencies can reach 87%, 91.6%, and 50.6% at 430, 532, and 633nm, respectively. This work combines the advantages of low-cost, semiconductor fabrication compatibility, and high efficiency that allow for miniaturization and integration of various optical components and applications, such as imaging sensors, high-resolution lithography, optical communications, and so on.

5. Tunable Metalenses

Metalenses discussed all have one feature in common, i.e., their properties are fixed once made. There is another impor-tant direction of research that is emerging, namely, the tun-able metalenses with functionalities that can be actively varied. Such actively variable functionalities are desirable in optical applications where versatility is required. To date, there are two common approaches that have been used to realize tunable metalenses. The first kind is based on reconfigurable metasur-faces.[85,86] The working principle of this category of metasur-faces relies on the ability to reconFigure physical dimensions of the metasurfaces including the interspace between the meta-atoms and reshaping the individual meta-atoms to actively


Figure 6. Novel applications of metalenses. a) Image of resolution test chart captured by a TiO2-based metalens with 530 nm illumination. The scale bars: 40 µm.[84] b) Images of the highlighted region in (a) at wavelengths of 480, 530, 590, and 620 nm, respectively. The scale bars: 5 µm. c) Image of resolution test chart taken from the GaN-based achromatic metalens. The scale bars: 4 µm.[81] d) Full-colour Erithacus rubecula images captured by the GaN-based achromatic metalens.[81] e) Schematic diagram of the off-axis metalens.[82] f) High spectral resolution at the focusing angle of 80°. A wavelength difference as small as 200 pm is resolved.[82] g) Schematic of a full-color routing metalens with light convergence and color filtering functionalities.[83] (a,b) Reproduced with permission.[80] Copyright 2016, American Association for the Advancement of Science. (c,d) Reproduced with permission.[74] Copyright 2018, Nature Publishing Group. (e,f) Reproduced with permission.[82] Copyright 2016, American Chemical Society. (g) Reproduced with permission.[83] Copyright 2018, American Chemical Society.




manipulate the output wavefront. With the change of the elec-tromagnetic coupling and the scattering phase difference due to the change of near-field interaction between meta-atoms, the resonance wavelength as well as the output wavefront of metasurfaces can be modulated accordingly. Another approach is to integrate active materials into the metalenses. Optical properties of semiconductors such as GaAs,[87] indium tin oxide (ITO),[88,89] phase-change materials,[49,90–92] and graphene[93–96] can be actively tuned by applying external excitation. Because the optical resonances of meta-atoms are highly sensitive to their dielectric background, by placing a metasurface nearby an active material, its optical response can be actively controlled as well. In this seciton, we will briefly review the progress made in the development of reconfigurable and tunable metalenes.

5.1. Stretchable Metalens

One of the most efficient ways to realize a tunable metalens is to integrate a metalens in a stretchable substrate. Stretch-able materials[97] such as polydimethylsiloxane (PDMS) have been widely used in reconfigurable photonic devices for color generation,[98,99] resonance switch,[100–108] and miniature spec-troscope[109] due to their high flexibility, reversibility, as well as stability. They are also inexpensive and can be prepared easily. The fabrication of stretchable metalenses is generally based on two steps: nanofabrication of a metalens on a tem-plate (Figure 7a) followed by the pattern transfer (Figure 7b). For example, Ee and Agarwal used e-beam lithography to fab-ricate a metalens consisting of gold/poly(methyl methacrylate) (PMMA) bilayered nanoparticles on a silicon substrate and casted a PDMS layer over it. By taking advantage of the poor adhesion between the PMMA and silicon, the metalens was successfully transferred to the stretchable substrate (Figure 7c). The function of the stretchable substrate is to change the inter-space of meta-atoms in the metalens to modulate the phase at the positions of individual meta-atoms. Faraon and co-workers found that the change of the phase profile along the stretch-able metalens is proportional to 1/(1+ε)2, where ε is the strain ratio of the stretchable substrate (Figure 7d).[110] As a result, the focusing spot of the metalens can be continuously moved along the axis by gradually changing the strain applied to the met-alens (Figure 7e).

The stretchable metalens can be integrated with electric actu-ators to work as an adaptive planar lens. Adaptive lenses are important in applications such as astronomical imaging, optical communication, and optical scanning microscope. However, current adaptive lenses are either too bulky[111] or highly sensi-tive to light polarization.[112,113] To address this issue, Capasso and co-workers reported an electrically stretchable metalens capable of not only shifting the focal spot in three dimen-sions but also dynamically correcting the astigmatism.[114] The proposed device is a combination of a metalens composed of silicon nanoposts and dielectric elastomer actuators, as shown in Figure 7f–i. To fabricate this device, the metalens was ini-tially made on a silicon wafer and subsequently transferred to an off-the-shelf acrylate elastomer (VHB Tape 4905, as the stretchable substrate). Between the metalens and the substrate, a single-walled carbon nanotube layer as optically transparent

electrode was patterned on the substrate prior to the met-alens transfer. The stretchable material used in this work is a type of electroactive polymer, which is sometimes referred to as artificial muscle.[97] It can compress along the direction of external bias,[97] therefore, when a vertical bias is applied on the polymer, it will expand laterally due to volume conserva-tion. The lattice constant of the metalens on the top can be manipulated by locally applying a bias on specific electrodes, resulting in local tuning of the phase profile accordingly. This enables the proposed metalens to adjust the output wavefront for various applications of adaptive optics. Figure 7g shows the results of focal length tuning from 50 mm to nominally 100 mm with a tuning ratio larger than 100%. The lateral shift of the focus spot as well as the active correction of the astig-matism are realized by applying a bias on specific electrodes, as shown in Figure 7h,i. Notably, because the meta-atoms in the device are circular nanoposts, this metalens is insensitive to the polarization state of the incident light. This makes it very useful in many applications that do not necessarily need polar-ized light but require high efficiency, such as astronomical and bioimaging systems.

5.2. Microelectromechanical Systems (MEMS)-Reconfigurable Metalens

MEMS have been functionally applied as a feasible approach to achieve reconfigurable metalenses. With MEMS tech-nology, reconfigurable metasurfaces for intensity and anisot-ropy switching have been demonstrated in optical[85] and THz regimes.[116–119] Recently, Faraon and co-workers reported a MEMS-based metalens doublet that its focal length can be continuously tuned along the optical axis.[120] Its fabrication flowchart and working principle are shown in Figure 8a,b, respectively. A pair of metalenses consisting of a-Si nanoposts are made on two substrates: one a freestanding silicon nitride substrate and the other a glass substrate. A spacer made of optical resist is inserted between the two metalenses to con-trol the interspace between them around 10 µm. Both are sur-rounded by metallic rings to form a vertical capacitor (Figure 8c). By applying a bias on the metallic rings, the interspace between two metalenses can be actively controlled, resulting in the dynamic change of the effect focal length (Figure 8d). A result of the imaging obtained using this MEMS-based metalens is also demonstrated. By carefully controlling the bias applied on the device, the metalens can generate an image that clearly reproduces the resolution chart as shown in Figure 8e.

5.3. Addressable GHz Metalens with Liquid Metal

As the wavefront tuning of MEMS-based metalenses is usu-ally obtained by varying the interspace of the meta-atoms or the metalens layers, this tuning is typically accompanied with some form of overall spatial variation of the devices which is not always desirable for some highly compact photonic devices in which the tolerance of such a spatial change is difficult. If the resonances of the meta-atoms can be individually tuned via their physical shape changes without the overall physical






Figure 7. Stretchable metalens. a) Left: As-fabricated gold metalens before being transferred to the stretchable substrates. Right: The scanning electron microscope (SEM) image of the template after the metalens was transferred. Scale bar: 400 nm. b) An example of nanostructure transfer technique. The metalens made on a Si substrate template can be transferred to the PDMS by taking advantage of the different substrate adhesion. c) A photograph of met-alens before and after being stretched. Scale bar: 10 mm. d) The working principle of the stretchable metalens for focal length tuning. e) Experimental optical intensity profiles of the strained metalens (made of Si nanoposts in a PDMS substrate) along the axial plane and the corresponding focal plane images. The focal length was tuned from 600 µm to around 1380 µm. Scale bar: 5 µm.[115] f) Photograph of the electrically stretchable metalens. Results of g) focal length tuning, h) 3D shifting the focal spot, as well as i) astigmatism correction. Scale bar: 20 µm. (a)–(c) Reproduced with permission.[115] Copyright 2016, American Chemical Society.[115] (d),(e) Reproduced with permission.[110] Copyright 2016, Wiley-VCH.[110] (f)–(i) Reproduced with permission.[78] Copyright 2018, American Association for the Advancement of Science.




variation of the metalens, the ultimate degree of freedom for dynamical wavefront manipulation can be achieved. To realize this, Liu and co-workers and Zheludev et al. developed a recon-figurable metalens consisting of microfluidic channels and liquid metal mercury. Liquid metals such as mercury and gal-instan have melting points at room temperature, and they have similar electrical conductivities as copper and aluminum. That makes them suitable to be used as active materials in metasur-face devices.[121–123] In the proposed metalens, mercury is filled in ring shaped microcavities (Figure 9a). By controlling the air pressure in a specific cavity via a pneumatic valve, a gap can be introduced in a meta-atom. The size and location of the air gap in the ring can be precisely controlled. As such, the ampli-tude and phase modulation by the individual meta-atom can be controlled (Figure 9b). The tuning of focus spot is shown in Figure 9c, where the corresponding phase profiles of the metalens consisting of different set of meta-atoms are shown in Figure 9d. As can be seen in Figure 9c, the focal length of this GHz planar metalens can be continuously tuned from 5λ to 15λ by modifying the spatial phase gradient along the met-alens. While the reported metalens worked in GHz regime, it can be scaled down to work in the optical regime by adopting nanofluidics.[124–126]

5.4. Tunable Metalenses with Phase-Change Material Alloys

Phase-change materials such as Ge2Sb2Te5 and AgInSbTe have been widely used in commercial rewritable and nonvolatile optical disks and as media for storage cells in electronic phase-change memories due to their large optical/electrical contrast

between amorphous and crystalline states.[49,90–92,128–133] The phase states of phase-change material thin films can be reversibly switched by applying laser/electrical pulses on them.[49,90–92,128,130,133,134] Recently, phase-change materials have been used in nanophotonic devices for optical switching,[135,136] active beam steering,[136] and color change displaying.[137] Phase-change materials can also be used in tunable metalenses due to their low loss from optical to mid-IR regime and fast phase-transition time.[132] For example, Giessen et al. reported a mid-IR tunable metalens comprising of a plasmonic nanorod array and a phase-change thin film. The plasmonic layer is a combination of two metalenses consisting of gold nanorods with different lengths (Figure 10a,b). When the phase-change layer is in the amorphous state, the metalens consisting of longer gold nanorods is in resonnace at the wavelength of 3.2 µm while the other set of nanorods with shorter length is off-resonance. When the phase-changing layer is switched to crystalline state, the metalens consisting of shorter nanorods is in resonance while the longer ones are off-resonance. Since the two metalenses are designed to have different phase profiles along the surface (Figure 10c), the focal length of this device can be switched by phase state change, as shown in Figure 10d. This category of tunable metalenses can be used to obtain mul-tifocal lengths when more metalenses are integrated into the plasmonic layer.

Phase-change material can not only serve as the active layer to tune the metalenses but also be used as a “canvas” for direct writing of metasurface on it.[91,138–140] Wang et al. demonstrated a tunable all-dielectric metalens using a pulsed femtosecond laser to record grayscale patterns consisting of crystalline nanomarks on an amorphous phase-change film


Figure 8. MEMS-tunable metalens. a) Fabrication process of the MEMS-tunable metalens. b) Working principle of the device. By controlling the inter-space between two metalenses, the effective focal length can be tuned accordingly. c) Photographs of the metalens pair. Gold rings as the vertical capacity can be seen in the images. Scale bars: 100 µm. d) Measured effective focal length versus the applied DC voltage of the metalens doublet. e) Applica-tion of the metalens doublet for imaging. The scale bars: 10 µm. (a)–(e) Reproduced with permission.[120] Copyright 2018, Nature Publishing Group.





(Figure 10e).[139] As shown in Figure 10f, two closely spaced super-oscillation metalenses capable of producing two focal spots in free space were recorded using the titghtly focused 780 nm femtosecond laser pulses. By carefully controlling the illumination parameters of the fs-laser pulses, the recorded metaleneses can be erased as well as rewritten on the phase-change thin film (the middle panel of Figure 10f). This result points to the potential of the phase-change metalenses for a range of on-demand applications, such as real-time optical scanning, imaging, and optical data processing.

6. Prospects and Conclusion

In this article, we have surveyed the recent development of the metalenses. One of the most exciting achievements is the realization of broadband achromatic metalenses with the use of integrated-resonant units. These metalenses can be made flat, compact, and integrated in other optical systems with great potential to replace their conventional bulky coun-terparts. With the design flexibility offered by the degrees of freedom to vary the geometrical parameters, interspace, and distribution of meta-atoms, metalenses can be made to per-form functionalities that are challenging to realize with con-ventional lenses, such as compact spectroscopy and full-color routing. However, there remaining significant challenges as metalenses are being improved to fulfill these potentials. For example, current broadband achromatic metalenses rely

on Pancharatnam–Berry phase method which only works for circularly polarized incident light. This property makes ach-romatic metalenses unsuitable in many practical applicaitons because of the need for extra components to convert inci-dent light into a cicularly polarized one. At the moment, the largest numerical aperture and best efficiency of the reported achromatic metalenses based on dielectric meta-atoms are 0.2 and 40%, respectively. Achromatic metalenses clearly need improvement to increase their performance, and to this end, novel working principles and more sophisticated design of meta-atoms need to be explored.

Metalenses can be integrated into a range of photonic devices to improve their performance and expand function-alities. For example, metalenses can be used in applications of vivo imaging for diagnosis due to their compact sizes and good imaging capability. In light of their better imaging quali-ties and much smaller footprint, metalenses can be used to replace microlens arrays in optical devices such as light field camera and hemispherical electronic eye camera to improve their performance and augment their functionalities.[142] The great scalabilty of metalenses also makes them possible to be integrated into tiny unmanned flying vehicles such as machine insects. Also, integrating metalenses with various functionali-ties on the ends of optical fibers can be very useful in optical communication applications. Many conventional diffractive optical elements can be replaced by them. Some interesting research directions of metalenses are also just emerging and have not been fully studied yet. For instance, metalenses

Figure 9. Liquid metal metalens. a) Photographs of the liquid metal metalens. The device is composed of ring-shaped microfluidic civilities filled with liquid metal mercury. The individual meta-atoms can be reshaped by controlling the pressure in the air gap. b) Phase and amplitude modulation of the mercury meta-atom in different shapes and orientations. By controlling the geometrical parameters of the meta-atom, 2π-phase modulation can be achieved. c) Experiment and simulation results of the focal spot shift of the proposed metalens device and d) the corresponding phase profiles of metalens with different sets of the meta-atoms. (a)–(d) Reproduced with permission.[127] Copyright 2015, Wiley-VCH.





working in the visible for nonlinear generation and focusing are recently reported.[143,144] Although their efficiencies are quite low at the moment, they can be improved and in due time serve as multifunctional devices for imaging and scanning if novel nonlinear materials (e.g., multiquantum-well semicon-ductor heterostructures)[145] of higher efficiency are integrated in the devices. Metalenses for manipulating thermal radiation are another interesting topic. A few reports studying the use of plasmonic metasurfaces to control thermal emission spectra have appeared recently,[146,147] pointing to their potential appli-cations in thermal imaging and focusing.

Another emerging area is the tunable metalenses enabled by the incorporation of structures or materials whose geom-etries or properties can be actively varied on demand. So far, majority of the metalenses in this area are demonstrated with reconfigurable structures where the interspace between meta-atoms and their shapes can be changed via various mechanical mechanisms enabled by means such as stretchable substrates, MEMS, and air presure that create gaps in liquid metal. Tun-able metalenses integrated with active materials that can be

actively controlled have begun to emerge, promising advan-tages such as being more compact with faster response time. At the moment, tunable metalenses incorporating active materials have only been demonstrated in the near-infrared regime. The next frontier would be to expand their working range to the vis-ible regime while achieving ultrafast tuning speed.

In conclusion, metalenses have already been ready to be used in a number of novel devices including portable mobile devices, virtual reality headsets, as well as drones. They are also expected to further penetrate and make impact to all kinds of optical systems. In light of their exotic optical functionalities enabled by their versatile wavefront tuning capability as well as ultrasmall sizes, metalenses could potentially revolutionize photonics and optoelectronics in the forseeable future.

AcknowledgementsM.L.T., H.-H.H., and C.H.C. contributed equally to this article. The authors acknowledge financial support from Ministry of Science and

Figure 10. Phase-change-material-based metalens. a–d) Plasmonic metalens on a phase-change thin film for dynamic focal length tuning.[141] a) SEM image of the metalens. Scale bar: 5 µm. b) Transmission spectra of rods on an amorphous (left panel) and crystalline (right panel) phase-change thin film. c) Phase profiles of the metalens in two phase states at the working wavelength. d) Dynamic focal length tuning with the tunable metalens. e) All-dielectric metalens recorded on a phase-change thin film. A metalens can be readily written on a phase-change thin film by using the femtosecond laser pulses.[139] f) Dynamically tuning the functionality of the phase-change metalens. A pair of metalenses was written on the phase-change thin film initially. Two super-resolution focusing spots can be produced by the metalens pair. After the right metalens was erased, only the left focusing spot can be observed. However, after the erased metalens was rewritten, two super-resolution spots can be observed again, indicating the reversibility of the metalens. Scale bar: 10 µm. (a)–(d) Reproduced with permission.[141] Copyright 2017, Nature Publishing Group. (e,f) Reproduced with permission.[139] Copyright 2016, Nature Publishing Group.





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 the 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 support. G. Sun acknowledges support from Air Force Office of Scientific Research (grant nos. FA9550-17-1-0354 and FA2386-17-1-4100). The authors thank Prof. Shuming Wang and Dr. Pin Chieh Wu for their useful discussions.

Conflict of InterestThe authors declare no conflict of interest.

Keywordsmetadevices, metalenses, metasurfaces, nanophotonic devices, planar optics

Received: April 28, 2018Revised: June 14, 2018

Published online:

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