Ruwen Peng’s research while affiliated with Nanjing University and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (81)


Schematic of the non-orthogonal arbitrary polarization-multiplexed metasurface. When the metasurface is illuminated and analyzed by three non-orthogonal arbitrary polarization combinations, three different holographic images can be generated independently.
Metasurface design. (a) Schematic of the single α-Si nanopillar. Simulated transmission (b) magnitude and (c) phase shift of the nanopillar with x-polarized incidence. (d) Schematic of the designed supercell. (e, f) Jones matrix elements of two different supercells as examples. The blue and red symbols represent FDTD results and calculated results, respectively. The three different shaped symbols represent the three Jones matrix elements.
Non-orthogonal linear polarization multiplexing metasurfaces. (a) The optical setup. (b) The optical and SEM micrographs of the copolarized multiplexing sample. The scale bars are 50 μm, 400 nm, and 1 μm, respectively. (c) Simulated and measured holographic images of the copolarized multiplexing sample. The scale bars are 25 μm. (d) The optical and SEM images of the non-copolarized multiplexing sample. The scale bars are 50 μm, 1 μm, and 1 μm, respectively. (e) Simulated and measured holographic images of the non-copolarized multiplexing sample. The scale bars are 25 μm. The white arrows in the top right corner represent the corresponding input and out polarizations.
Circular polarization multiplexing metasurfaces. (a) The optical and SEM micrographs of the sample. The scale bars are 50 μm, 1 μm, and 1 μm, respectively. (b) Simulated and measured holographic images. The scale bars are 25 μm.
Non-orthogonal elliptical polarization multiplexing. The optical micrographs, SEM micrographs and measured holographic images of (a) the copolarized multiplexing and (c) the non-copolarized multiplexing sample. The scale bars are 50 μm, 2 μm, 50 μm, and 10 μm, respectively. The white arrows in the top right corner represent the corresponding incident and analyzed polarizations. Measured correlation coefficients matrix of (b) the copolarized multiplexing and (d) the non-copolarized multiplexing sample.

+3

Metasurface-based non-orthogonal tri-channel polarization multiplexing for optical encryption [Invited]
  • Article
  • Full-text available

February 2025

·

32 Reads

Yu Liu

·

Xing-Yuan Huo

·

Yu-Tong Xiao

·

[...]

·

Orthogonal polarization multiplexing is typically required to avoid crosstalk between channels. However, for practical applications in optical information encryption, orthogonal polarization channels are vulnerable to decoding. Using non-orthogonal polarization channels can enhance information security. Here, we extend the conventional Jones matrix approach to achieve non-orthogonal tri-channel polarization multiplexing metasurfaces for optical encryption via optical holography. Using a supercell configuration with two pairs of α-Si meta-atoms, we experimentally demonstrate metasurface-based multiplexing under three linear polarization channels, including copolarized and non-copolarized channels. This design strategy is further extended to circular and elliptical polarization channels, which exhibits minimum crosstalk. As a proof-of-concept demonstration, we implement two optical encryption applications, i.e., image encryption and character encryption, based on non-orthogonal polarization-multiplexed metasurfaces. For image encryption, encrypted images are generated only in the correct polarization channels. While using seven different statuses of metasurface under various polarization channels, we also present a character encryption scheme. We envision that the non-orthogonal polarization multiplexing metasurface platform will open new possibilities in optical communication, optical encoding, and information security.

Download

Metasurface polarization optics: From classical to quantum

December 2024

·

377 Reads

·

4 Citations

Metasurface polarization optics, manipulating polarization using metasurfaces composed of subwavelength anisotropic nanostructure array, has enabled a lot of innovative integrated strategies for versatile and on-demand polarization generation, modulation, and detection. Compared with conventional bulky optical elements for polarization control, metasurface polarization optics provides a feasible platform in a subwavelength scale to build ultra-compact and multifunctional polarization devices, greatly shrinking the size of the whole polarized optical system and network. Here, we review the recent progresses of metasurface polarization optics in both classical and quantum regimes, including uniform and spatially varying polarization-manipulating devices. Basic polarization optical elements such as meta-waveplate, meta-polarizer, and resonant meta-devices with polarization singularities provide compact means to generate and modulate uniform polarization beams. Spatial-varying polarization manipulation by employing the pixelation feature of metasurfaces, leading to advanced diffraction and imaging functionalities, such as vectorial holography, classic and quantum polarization imaging, quantum polarization entanglement, quantum interference, and modulation. Substituting conventional polarization optics, metasurface approaches pave the way for on-chip classic or quantum information processing, flourishing advanced applications in displaying, communication, imaging, and computing.


Simulation study of flexible wavefront shaping in Smith-Purcell radiation with aperiodic metagratings

September 2024

·

49 Reads

Smith-Purcell radiation (SPR) is a versatile platform for finely tuning nanoscale light across a broad spectral range. This study introduces a theoretical approach for shaping SPR wavefronts using aperiodic metagratings (AMGs). The AMGs consist of arrays of identical metal nano-rods (MNRs), with each MNR's spatial position precisely adjustable. This precise adjustment allows for effective modulation of the spatial phase distribution of SPR. To demonstrate the efficacy of this method, we conduct simulations to achieve diverse wavefront profiles of focusing, deflection, Bessel beams, and Airy beams. Additionally, our approach allows for integrating multiple SPR wavefront functionalities within a combo AMG. By employing the asymmetric L-shaped meta-atom design, we achieve simultaneous SPR polarization conversion and wavefront shaping. This method is promising for developing highly adaptable and multifunctional nanoscale light sources.


Fig. 2 Design of effective self-dual MMs using dielectric multilayers. a Illustration of a dielectric MM consisting of ABA multilayers. b Transmittance through N numbers of ABA units in air as a function of the incident angle θ i for TE (blue) and TM (red) polarizations. c Wave impedances of free space (lines) and MM (dots) for TE and TM polarizations. d Band structures of the MM for TE (blue) and TM (red) modes. The black dashed line denotes the functioning frequency fa=c ¼ 0:277. e EFSs of TE (blue) and TM (red) modes at fa=c ¼ 0:277. f Angle of refraction θ r at the interface between free space and MM as a function of the incident angle θ i for TE (blue) and TM (red) polarizations
Fig. 3 Effective self-duality-induced birefringence-free anisotropy. Illustration of circularly polarized waves incident upon (a) a conventional anisotropic dielectric slab, (c) an anisotropic pure-dielectric MM slab. Simulated distributions of E y (upper) and H y (lower) for a circularly polarized Gaussian beam incident upon (b) an anisotropic dielectric A slab with a thickness of 10a, or (d) an anisotropic pure-dielectric MM slab with 10 unit cells under θ i ¼ 60° and fa=c ¼ 0:277. The angle of refraction θ r within the A and MM slabs is indicated
Fig. 4 Experimental observation of full-polarization omnidirectional Brewster effect. a Illustration of the unit cell of the designed MM consisting of different alumina layers spaced by foam. b Picture of the fabricated sample with a unit cell and the measuring environment. c Simulated transmittance through the MM sample (solid lines and symbols) and an alumina slab of the same thickness (dashed lines) for TE (blue) and TM (red) polarizations as a function of the incident angle at 3.8 GHz. d Measured E y on the xz (upper) and yz (lower) planes at 3.8 GHz. The left, middle and right panel graphs denote the case of the MM sample, the case of free space and the case of the alumina sample, respectively. Scattered fields in the cases of the MM (left) and pure alumina (right) samples on the (e) xz and f yz planes on the source side
Fig. 5 Totally wave-transparent MM radomes. Simulated distributions of electric (upper) and magnetic (lower) fields radiated from out-of-plane electric (upper) and magnetic (lower) monopolar sources, placed off-center within a circular (a) MM, (b) dielectric radome. The MM radome is composed of a single ABA unit, adopted from Fig. 2, and the dielectric radome is made of pure dielectric B. The two radomes have the same total thickness. c Far-field radiation patterns without any radome (cyan), with a MM radome (red), with a dielectric radome (black) for the cases of out-ofplane electric (upper) and magnetic (lower) monopolar sources. The functioning frequency is 8.30 GHz
Dielectric metamaterials with effective self-duality and full-polarization omnidirectional brewster effect

September 2024

·

135 Reads

·

3 Citations

Light Science & Applications

Conventional dielectric solid materials, both natural and artificial, lack electromagnetic self-duality and thus require additional coatings to achieve impedance matching with free space. Here, we present a class of dielectric metamaterials that are effectively self-dual and vacuum-like, thereby exhibiting full-polarization omnidirectional impedance matching as an unusual Brewster effect extended across all incident angles and polarizations. With both birefringence and reflection eliminated regardless of wavefront and polarization, such anisotropic metamaterials could establish the electromagnetic equivalence with “stretched free space” in transformation optics, as substantiated through full-wave simulations and microwave experiments. Our findings open a practical pathway for realizing unprecedented polarization-independence and omnidirectional impedance-matching characteristics in pure dielectric solids.


Schematic diagram of dewdrops in nature and tunable dewdrop metasurfaces. The states of the dewdrop metasurfaces can be modulated by the substrate surface properties as well as by the environmental temperature and relative humidity.
Preparation of dewdrop metasurfaces and principle of unit cell manufacture. a) Fabrication processes of dewdrop metasurface using hydrophobic nanoparticles spray coating treatment. The pattern mask blocks hydrophobic nanoparticles from depositing on hydrophilic patterns. b) Side view of real‐time controlled dewdrop condensation and evaporation devices. c) Various dewdrop patterns condensed on hydrophilic/hydrophobic hybrid dewdrop metasurfaces, and all of the scale bars represent 5 mm.
Tunable ultrabroadband absorption based on a TDM. a) Schematic of the meta‐atom of the TDMs. b) Photographs of ultrabroadband absorption TDMs under different ambient conditions, and the scale bar is 10 mm. c,d) Simulation and experimental results of the absorption spectrum c) under different temperature differences between Ta and Ts and d) different RH.
A tunable binary‐phase grating enabled by the TDM. a) Schematic of the meta‐atoms of the TDM. b) A tunable binary‐phase grating composed of meta‐atom I and II. c) Zoomed‐in view of fabricated TDM in two different states with and without dewdrops. d) Simulated electric‐field distribution of the TDM under normal incidences with y‐polarization at 14 GHz. Hollow arrows represent the incident beams. e) Simulated and f) measured far‐field scattering patterns of the TDM without and with dewdrops at 14 GHz.
Dewdrop Metasurfaces and Dynamic Control Based on Condensation and Evaporation

August 2024

·

192 Reads

·

1 Citation

Dewdrops, the droplets of water naturally occurring on leaves and carapaces of insects, are a fascinating phenomenon in nature. Here, a man‐made array of dewdrops with arbitrary shapes and arrangements, which can function as an electromagnetic metasurface, is demonstrated. The realization of the dewdrop array is enabled by a surface covered by a tailored pattern of hydrophilic and hydrophobic coatings, where tiny droplets of water can aggregate and form dewdrops on the former. Interestingly, this metasurface made of dewdrops can be modulated by the condensation and evaporation process. By increasing relative humidity and decreasing temperature, the dewdrop metasurface is gradually formed with increasing amounts of water. While the reverse operation can make it completely disappear. This idea is demonstrated through two examples with different functions of dynamically controllable microwave absorption and scattering. The work shows a principle to construct functional electromagnetic devices with dewdrops, as well as a mechanism of dynamic control based on condensation and evaporation, promising unprecedented applications.



Matte surfaces with broadband transparency enabled by highly asymmetric diffusion of white light

March 2024

·

206 Reads

·

17 Citations

Science Advances

The long-standing paradox between matte appearance and transparency has deprived traditional matte materials of optical transparency. Here, we present a solution to this centuries-old optical conundrum by harnessing the potential of disordered optical metasurfaces. Through the construction of a random array of meta-atoms tailored in asymmetric backgrounds, we have created transparent matte surfaces that maintain clear transparency regardless of the strength of disordered light scattering or their matte appearances. This remarkable property originates in the achievement of highly asymmetric light diffusion, exhibiting substantial diffusion in reflection and negligible diffusion in transmission across the entire visible spectrum. By fabricating macroscopic samples of such metasurfaces through industrial lithography, we have experimentally demonstrated transparent windows camouflaged as traditional matte materials, as well as transparent displays with high clarity, full color, and one-way visibility. Our work introduces an unprecedented frontier of transparent matte materials in optics, offering unprecedented opportunities and applications.


Fig. 1. Dielectric MM exhibiting effective self-dual property and full-polarization omnidirectional Brewster effect. a The classical Brewster effect limited to a particular incident angle, i.e. Brewster's angle í µí¼ƒ b and the TM polarization, and the birefringence effect of beam splitting due to anisotropy. b Illustration of an anisotropic dielectric MM exhibiting full-polarization omnidirectional Brewster effect, as well as birefringence-free anisotropy as the consequence of effective duality symmetry realized in this dielectric MM.
Fig. 4. Experimental observation of full-polarization omnidirectional Brewster effect. a Illustration of the unit cell of the designed MM consisting of different alumina layers spaced by foam. b Picture of the fabricated sample with a unit cell and the measuring environment. c Simulated transmittance through the MM sample (solid lines and symbols) and an alumina slab of the same thickness (dashed lines) for TE (blue) and TM (red) polarizations as a function of the incident angle at 3.8GHz. d Measured í µí°¸íµí°¸í µí±¦ on the í µí±¥í µí± § (upper) and í µí±¦í µí± § (lower) planes at 3.8GHz. The left, middle and right panel graphs denote the case of the MM sample, the case of free space and the case of the alumina sample, respectively. Scattered fields in the cases of the MM (left) and pure alumina (right) samples on the e í µí±¥í µí± § and f í µí±¦í µí± § planes on the source side.
Dielectric Metamaterials with Effective Self-duality and Full-polarization Omnidirectional Brewster Effect

March 2024

·

230 Reads

Conventional dielectric solid materials, both natural and artificial, lack electromagnetic self-duality and fail to achieve impedance matching with free space. Here, we present a class of dielectric metamaterials that exhibit effective self-duality and also enable full-polarization omnidirectional impedance matching, thereby extending the Brewster effect across all incident angles and polarizations. The self-duality eliminates birefringence despite significant anisotropy in dispersion. Meanwhile, the full-polarization omnidirectional Brewster effect ensures near-zero reflection on interfaces with free space, regardless of incidence wavefront and polarization. These unique properties establish electromagnetic equivalence with "stretched free space" in transformation optics, as substantiated through full-wave simulations and microwave experiments. Our findings open a pathway for realizing unprecedented polarization-independence and omnidirectional impedance-matching characteristics in pure dielectric solids.


The schematics of a metasurface for THG via GMR, which consists of a parallel array of notched waveguides. The separation of the waveguides p is 580 nm, the waveguide height h = 500 nm, and the width w = 300 nm. The notches on the silicon waveguides are arranged along the y-axis, with notch period L= 500 nm for MS1 and L= 550 nm for MS2. The notch sizes nx and ny are 80 and 60 nm, respectively.
Simulations of the guided mode resonances. (a) Numerically calculated transmittance for various notch periodicity L with fixed notch size nx = 80 nm and ny = 60 nm. The incident light is x-polarized. The stars labeled MS1 and MS2 represent two waveguiding modes with L as 500 and 550 nm, respectively. The resonant modes are TE21 and TE13, accordingly. (b) and (c) Simulated electric field distribution of structure MS1 viewed on x-z and x-y planes, respectively. (d) and (e) Simulated electric field distribution of MS2 viewed on x-z and x-y planes, respectively. The color bar |E|/|E0| in (b)–(e) labels the normalized amplitude of the electric field with respect to the incidence. The white arrows represent the in-plane electric field vectors.
SEM micrographs and transmission spectra of the fabricated metasurfaces. (a) and (b) SEM micrographs of the fabricated metasurfaces MS1 and MS2. The inset shows the oblique view of the samples. (c) and (d) Simulated and measured the white-light transmission spectrum of MS1 and MS2. The inset shows the schematic of the transmission on the metasurface by normal incidence. For MS1, a resonant dip appears at 1031.4 nm in simulation and experimentally occurs at 1033.3 nm. For MS2, a dip appears at 1033.2 nm in simulation and occurs at 1036.8 nm in the experiment. The incidence is x-polarized. The full width at half maxima of the resonance is 7.5 nm for MS1 and 9.5 nm for MS2. The gray areas in (c) and (d) highlight the resonance locations.
Measurement of THG signal from the metasurfaces. (a) Experimental setup for THG measurement from the metasurface. (b) The normalized spectra of the fundamental pump laser (red) and the THG (purple) generated from the metasurface. (c) Measured THG spectrum from the metasurfaces and that from a flat silicon film of the same thickness. The pump power is 2.72 mW on metasurface MS1 (orange) and MS2 (blue) and 0.13 W on the silicon film (gray). The integration time is 10 s on the metasurfaces and 90 s on the silicon film. The magnification factor of 10⁶ in (c) is calculated from the pump power and integration time values in the measurements. (d) and (e) THG power dependence of the metasurfaces MS1 and MS2. The insets in (d) and (e) show the THG conversion efficiency as a function of average pump power. The maximum THG conversion efficiency reaches 7.71 × 10⁻⁵ in MS1 and 4.15 × 10⁻⁵ in MS2. The fitted exponent values from the data are 2.949 ± 0.015 for MS1 and 2.963 ± 0.018 for MS2.
Giant enhancement of third harmonic generation via guided mode resonances in notched silicon waveguides

March 2024

·

95 Reads

·

2 Citations

We report a giant enhancement of the third harmonic generation (THG) at 343 nm by periodically notched silicon waveguide arrays supporting guided mode resonances (GMRs) at 1030 nm. Maximum efficiency of the third harmonic generation η = 7.71 × 10⁻⁵ is achieved with a peak pump power density of 5.31 GW/cm². The enhancement factor of the THG from the GMR metasurface reaches up to 1.3 × 10⁷ compared to a flat silicon film with the same thickness. This observation demonstrates a promising approach to design high-efficiency nonlinear optical metasurfaces.


(a) Schematic shows the metasurface structures, where the asymmetric unit cell consists of two cuboids with different lengths. (b) Reflectance under the incidence of polarized light in the x-direction versus asymmetry parameter α (horizontal axis) and wavelength (vertical axis). (c) Q-factor (blue solid line) of the designed BIC and eigenmode wavelength (dashed line) as a function of α. (d) Electric field inside the two Si cuboids for the accidental BIC when α is around 0.21. The electric field vector is shown with black arrows. (e) Near-field distributions of the electric and magnetic fields of the accidental BIC when α is around 0.21.
(a) Top view and 45° tilted-angle (inset) SEM images of the fabricated Si metasurface placed on a fused silica substrate. (b) Evolution of the simulated (left) and measured (right) reflectance spectra versus asymmetry parameter α (0.15, blue; 0.18, red; 0.21, green; 0.23, yellow; 0.26, cyan).
(a) Schematics of the experimental setup to measure the THG reflectance. HWP, half-wave plate; DM, dichroism mirror; SF, short pass filter; P, powermeter. (b) Normalized spectrum of the fundamental pump laser (c) Normalized spectrum of the THG signal generated from the Si metasurface. The dashed red lines in (b) and (c) show the Gaussian curve fitting. (d) Experimentally measured dependence of the THG intensity with respect to the asymmetry parameter α. (e) Log–log plot of the output THG power as the function of the average pump power and the peak pump intensity for the Si metasurface with α = 0.21. The red dots show the measured data and the black dashed line is a numerical fit with a third-order power function. The yellow area covers the pump power range where the cubic law has been deviated. (f) Measured THG enhancement of the Si metasurface with respect to the signal from an unpatterned silicon film (magnified by 10⁶ times).
Realizing high-efficiency third harmonic generation via accidental bound states in the continuum

February 2024

·

155 Reads

·

12 Citations

The bound states in the continuum (BICs) have attracted much attention in designing metasurface due to their high Q-factor and effectiveness in suppressing radiational loss. Here we report on the realization of the third harmonic generation (THG) at a near-ultraviolet wavelength (343 nm) via accidental BICs in a metasurface. The absolute conversion efficiency of the THG reaches 1.13 × 10⁻⁵ at a lower peak pump intensity of 0.7 GW/cm². This approach allows the generation of an unprecedentedly high nonlinear conversion efficiency with simple structures.


Citations (50)


... Utilizing this unique functionality, a miniaturized and simplified two-photon polymerization (TPP) system was developed and demonstrated efficient multi-focus parallel processing [13] . Wavelength and polarization information can be independently encoded into each focal point, enabling the development of compact spectrometer [14] and polarization-resolved device [15] . More importantly, metalensbased optical trapping arrays have emerged as a powerful platform for the preparation and manipulation of ultracold atoms [16,17] , enabling multifunctional control in complex quantum information experiments. ...

Reference:

Scalable manufacturing of polarization-insensitive metalenses with high-uniform focal arrays in the visible
Metasurface polarization optics: From classical to quantum

... This design principle, validated by both numerical simulations and proof-ofconcept experiments, offers a promising path for developing high-efficiency radiation from dielectrics beyond the critical angle. Compared with previous works of PAMs for small angles limited within the critical angle [22], [23], our work breaks the bottleneck of TIR, and opens a practical route towards unprecedented dielectric devices with omnidirectional high-efficiency [20], [46], [47]. Such reciprocityenabled designs [26]- [30] may inspire future innovations in advanced metasurface technologies. ...

Dielectric metamaterials with effective self-duality and full-polarization omnidirectional brewster effect

Light Science & Applications

... Hyperbolic materials have attracted significant interest for controlling light at the nanoscale [1-3], due to their intrinsic hyperbolic dispersion and strong electromagnetic field confinement [4]. They have been shown to support surface polaritons [5][6][7][8][9][10][11][12][13], with long-range and low-loss propagation of subwavelength information [8,11], guided waves [14][15][16][17], and negative refraction [4,5,[18][19][20]. In these materials, hyperbolic dispersion results from the principal elements of the permeability or permittivity tensor possessing opposite signs [4,5,8,11,16,[21][22][23][24]. ...

Cladding-Free Hyperbolic Waveguide Arrays
  • Citing Article
  • May 2024

ACS Photonics

... As shown in Figure 2c, under the incidence at an angle ′ i from the side of n 2 , this PAM can deflect the refractive beam to an angle of refraction ′ t > C with high efficiency. Interestingly, since the whole system is reciprocal, the reciprocity principle guarantees that when the incidence channel is switched with the transmission channel, the transmission coefficient is exactly the same, i.e., t ′ = t [28], [29]. Hence, when a beam is incident from the side of n 1 on the PAM at the angle of i = ′ t > C , the beam should be deflected to the angle of t = ′ i in the side of n 2 , as schematically shown in Figure 2d. ...

Matte surfaces with broadband transparency enabled by highly asymmetric diffusion of white light
  • Citing Article
  • March 2024

Science Advances

... More recently, metasurfaces-based terahertz wavefront manipulation devices have been developed [13,14]. Furthermore, the high-Q quasi bound states (q-BIC) of nonlinear metasurfaces can enhance strong fields and have wide applications in sensing [15][16][17], high harmonic generation [18][19][20], and nonlinear enhancement [21]. However, the high-Q q-BIC of nonlinear metasurfaces can effectively enhance nonlinear effects and provide a way to achieve non-reciprocal transmission with smaller external excitation light intensity. ...

Realizing high-efficiency third harmonic generation via accidental bound states in the continuum

... Previously, such a mechanism has led to the realization of "invisible" surfaces [22] and through-wall wireless communications [23], but those functions were still limited by the critical angle, due to the failure of traditional metasurface design strategy under the TIR condition. In order to circumvent the limitation of TIR, here we apply the reciprocity principle [24], [25], which has recently led to the discoveries of anomalous Brewster effect [26], [27] and transparent matte surfaces [28]- [30], in the metasurface design. As a result, a PAM working in microwave frequencies has been designed and experimentally fabricated, validating the phenomenon of high-efficiency radiation beyond the critical angle. ...

Programmable flip-metasurface with dynamically tunable reflection and broadband undistorted transmission

... Zero-index materials (ZIMs), characterized by near-zero permittivity and/or permeability, represent a unique class of materials exhibiting extraordinary properties, such as infinitely long wavelengths and zero phase advancement [1][2][3][4]. These distinctive features have facilitated numerous novel phenomena and applications, including tunneling waveguides [5][6][7][8][9], radiation and flux control [10][11][12][13][14], photonic doping and anti-doping [15][16][17][18][19][20][21][22][23][24][25], the enhancement and quenching of optical nonlinearity [26][27][28][29][30][31][32][33], and zero Minkowskicanonical momentum [34], etc. ZIMs have been realized across a wide range of frequencies, spanning from microwave to terahertz, infrared, and visible spectra, through the use of plasmonic materials at plasma frequencies [26,[35][36][37][38][39][40][41][42][43], non-resonant metal-dielectric composites [44,45], resonant metamaterials [7,14,24,46], waveguide metamaterials at cutoff frequencies [6,8,13,47,48], and photonic crystals (PhCs) [18,24,25,[49][50][51][52][53][54][55][56][57][58], etc. Despite these achievements, most practical implementations of ZIMs rely on metallic components or plasmonic materials, leading to significant material losses at high frequencies. ...

Crosstalk prohibition at the deep-subwavelength scale by epsilon-near-zero claddings

... The evolution of photon propagation science to a practical technology promises extreme advantages for specific applications in integrated optical circuits [5][6][7] , nano-antennas [8][9][10][11][12] , nanolasers [13][14][15] , etc. In the development of photon manipulation technology, it is substantial to find a proper method with features of high-level integration and a large storage capacity, to satisfy the need for information transmission and processing applications [16][17][18][19] . Facing these requirements, color science with multiple frequency channels provides a promising approach to achieving large information-encoding capacity, and steering photon momentum at nanoscale has been demonstrated to be ascendant in compact information devices [20][21][22] . ...

Breaking the limitation of polarization multiplexing in optical metasurfaces with engineered noise
  • Citing Article
  • January 2023

Science

... Wang et al. successfully developed a broadband photodetector that leveraged a HOIP (hybrid organic-inorganic perovskite) metasurface, as shown in Fig. 9(c). 121 The metasurface was prepared by precisely etching the as-grown MAPbI 3 perovskite film through a dual-beam focused ion beam system. The introduction of the HOIP metasurface along with the black reflective mirror resulted in a photocurrent enhancement exceeding 10 times across the UV to visible light region. ...

Improving Photoelectric Conversion with Broadband Perovskite Metasurface
  • Citing Article
  • August 2022

Nano Letters