2.1.

Plasmonic-Based Structural Colors

When light of a specific wavelength impinges on a metal surface, the phenomenon of collective oscillation between the free electrons on the metal surface and photons is known as SPs^[69]. SPs exhibit a strong near-field enhancement effect and in-plane momentum. With the rapid development of micrometer and nanometer manufacturing processes, subwavelength nanostructures based on SP have been successfully fabricated. In the field of nanophotonics, the plasmonic metasurface has become a transformative technology, enabling unprecedented control of light at the nanoscale^[70,71]. These two-dimensional arrays composed of nanostructured metal elements exploit the unique optical properties of plasmonic materials, especially noble metals like gold (Au) and silver (Ag)^[72,73]. Plasmonic metasurfaces can manipulate surface plasmon resonance (SPR), achieving precise control over the phase, amplitude, and polarization of light^[74–77]. This level of control has paved the way for numerous applications, including waveguides^[78,79], metalenses^[80], holography^[81], and wavefront modulation^[82,83]. One particularly fascinating application is the realization of structural color^[69].

Throughout history, people have known that metal nanoparticles can produce remarkable colors. Over 1700 years ago, Roman artisans created the famous Lycurgus Cup^[84] by mixing nano-sized metal particles into glass. Due to the strong modulation effect of SPR on electromagnetic waves, there have been numerous reports of high spatial resolution color filters based on SPR^[49,85,86]. In addition to classical plasmonic metasurfaces, researchers have also designed new nanostructures such as gap plasmons^[87] and Fabry-Pérot (FP) cavities^[88–90], and this section will briefly discuss them.

In the past decade, structural colors based on metal metasurfaces have been extensively researched. In the early stages, structural colors of metal nanostructures with different geometric shapes, materials, and arrangements were widely investigated^[91–97]. Transmission-type structural colors were achieved using metal grating structures through a subtractive method or by employing metal nano-hole arrays with different shapes and periods for transmission-based RGB colors^[98]. Additionally, reflective structural colors based on metal nanostructures, such as nanodisks made of Au or Ag, demonstrated vibrant color displays with only a $2\times 2$ array due to the strong LSPR effect, as shown in Fig. 3(a)^[42]. Reflective structural colors were also achieved using anisotropic nano-hole structures, as illustrated in Fig. 3(b), where a cross-shaped hole array on a 100 nm thick aluminum (Al) film exhibited color responses under different polarizations^[99]. While structural color design based on metal structures allows for ultrahigh spatial resolution (over $1.2\times {10}^5$ PPI)^[100], challenges such as achieving high brightness, wide color gamut distribution, and process complexity remain unresolved, significantly limiting the practical applications of metal metasurface structural colors. In recent years, researchers have addressed these challenges by proposing innovative structural designs and process solutions.

Fig. 3

Early designs of structural colors based on metal nanostructures. (a) Reflective structural color achieved with an array of Ag nanorods, requiring only a $2\times 2$ array for distinguishable pixels^[42]. (b) Anisotropic cross-shaped nanoapertures for polarization-sensitive transmissive structural color^[99].

Hail et al. designed an RGB structural color based on a plasmonic nanorod array, where the nanorods, composed of Ag, had a longitudinal axis in the y-direction with a periodicity of $Px=\lambda /n$ along the x-direction. Color tuning was achieved by adjusting the dimensions and periodic parameters of the nanorods, as illustrated in Fig. 4(a) (1)^[101]. Furthermore, at a fixed periodicity, simple control over nanorod size enabled independent adjustments in color brightness, as depicted in Fig. 4(a) (2). Figure 4(a) (3) demonstrates the blended spectra produced by mixing different primary color nanostructures, showcasing the potential for an infinite color palette through precise control of nanostructures. This design allows for ultra-smooth transitions in both color and brightness.

Fig. 4

Plasmonic structural color design for high-performance display. (a) Design using Ag nanorods for high-color saturation display (1), brightness control by adjusting nanorod size (2), and color tuning through the arrangement of structures with different wavelength responses (3)^[101]. (b) Schematic of high-performance structural color based on Ag nano-grooves for achieving complete control over brightness and color (1), (2), application of polarization response for advanced optical steganography (3), and achieving soft color displays through brightness variation (4)^[102].

Xu and coworkers achieved high-performance plasmonic structural color through plasmonic resonance, manifesting an enhanced 90° optical rotation due to birefringence^[102]. The metapixel is designed as an anisotropic nanogroove array embedded in an optically thick silver film, as shown in Fig. 4(b) (1). In experiments, Si mold was initially prepared using traditional electron beam lithography (EBL) and reactive ion etching (RIE). Subsequently, an Ag layer was deposited on the Si template, and the desired samples were obtained after peeling. The prepared Si mold can be reused for a long time and is suitable for large-scale industrial production. The standard structural parameters of the nanogrooves are set to length (l) = 200 nm, width (w) = 60 nm, thickness (h) = 40 nm, and period (p) = 160 nm. The resonance wavelength is controlled by adjusting the structural parameters using a scaling factor (s). Figure 4(b) (2) displays the reflection cross-polarized spectra with S factors ranging from 1.0 to 2.65, covering the entire visible spectrum. Additionally, the color brightness of this plasmonic metasurface can be independently controlled by adjusting the rotation angle $\alpha$ between incident linearly polarized (LP) light and nano-grooves, as shown in Fig. 4(b) (3). Due to the sensitive response to orthogonally polarized light, as shown in Fig. 4(b) (4), the authors further applied it to advanced optical steganography. Using non-oriented nanogrooves to graphically represent information, specific information can only be read by specific incident LP light and a polarization analyzer, achieving advanced optical encryption. However, despite the high-performance structural color achieved by this plasmonic metasurface using polarization conversion, it is severely hindered by the requirement for LP light and a polarization analyzer. Another noteworthy issue is its sensitivity to the incident angle, severely limiting its practical applications.

Furthermore, the FP cavity structure formed by sandwiching a dielectric material between two metal films has been widely studied as a relatively simple structure in the field of structural colors^{[88,103–108]}. In general, the transmission and reflection modes of FP cavities are typically determined by the phase shift propagated within the cavity, and this phase shift is influenced by the refractive index of the dielectric material, the thickness of the dielectric layer, and the angle of incident light. Therefore, various colors across the entire visible spectrum can be easily achieved by adjusting the thickness of the dielectric layer. However, due to the fact that the angle of incidence changes the path of light in the FP cavity, it exhibits different resonant wavelengths at different angles of incidence and rainbow colors in color, resulting in small observation angles.

To overcome the problem of different colors corresponding to different FP cavity lengths, Wei et al. embedded Si nanostructures into a FP cavity, achieving tunable transmission structural colors across the entire visible spectrum within a fixed cavity length^[109]. The structure, as shown in Fig. 5(a) (1), consisted of a Si nanoblock array encapsulated by two layers of 35 nm thick Ag films filled with PMMA. Control over the geometric dimensions and periodicity of the Si nanoblocks allowed for precise tuning of the response wavelength, resulting in a color gamut covering 194% of sRGB. Additionally, the mixing of nanostructures with different sizes enabled color blending capabilities, as illustrated in Fig. 5(a) (2). Furthermore, the embedded nanostructures introduced flexible polarization control, allowing for polarization-multiplexed FP structural colors by adjusting the responses of meta-atoms to different polarizations, as depicted in Fig. 5(a) (3).

Fig. 5

Structural color design based on FP cavity. (a) Integration of Si nanostructures into FP cavity for uniform cavity length structural color display (1), color tuning through the mixture of different nanostructures on a high-color-saturation display foundation (2), and easy achievement of polarization response by controlling the symmetry of nanostructures (3)^[109]. (b) Schematic structure of FROCs formed by two coupled light absorbers (1), deposition of an absorbing medium on the FP cavity, coupling of the upper broadband mode with the lower FP resonance to form Fano resonance, resulting in vivid structural colors (2), (4), and exhibiting over 50° observation angle (3)^[110].

Recently, Mohamed et al. designed a structure called Fabry-Perot resonance optical coatings (FROCs)^[110]. They deposited a layer of absorbing dielectric material on an FP cavity, where the absorbing medium forms a broadband absorbing cavity with the first metal layer, and the lower three layers form an FP resonance serving as a narrowband absorbing cavity. The coupling between the two resonant cavity modes exhibits Fano resonance, as shown in Fig. 5(b) (1). The optimized structure of FROCs consists of a 15 nm thick germanium (Ge) lossy layer, a 20 nm thick Ag layer, a ${\mathrm{TiO}}_2$ lossless layer, and a 100 nm Ag layer from top to bottom. The thickness of the ${\mathrm{TiO}}_2$ dielectric layer increases from 30 to 130 nm, achieving visible light coverage of the resonant wavelength. To further suppress the reflection at shorter wavelengths, a 50 nm layer of ${\mathrm{SiO}}_2$ was deposited on top of FROCs as a refractive index matching layer, achieving a 61% coverage of the CIE color space. The colors and CIE coordinates for FP cavities, FROCs, and FROCs with deposited silica are shown in Figs. 5(b) (2) and 5(b) (3). In contrast to the structural colors of FP cavities, FROCs exhibit reflective colors over a larger range of observation angles, demonstrating significant color stability from 0° to 50°, as depicted in Fig. 5(b) (4). The design of FROCs solves the problem of poor color saturation and small observation angle in FP cavities, and amorphous silicon can be used to replace Ge as the absorption layer, and the metal layer in the structure can be used as the electrode to achieve color photovoltaic cells.

On the basis of the FP cavity, further patterning the top metal film forms a nanostructure array, allowing for the adjustment of structural colors through the shape and size of the nano-units^[89,111,112]. The top metal nanostructures, in conjunction with the ultra-thin dielectric layer, constitute a metal-insulator-metal (MIM) structure that exhibits gap plasmons. This phenomenon arises due to the strong near-field coupling between the plasmonic modes of the top nanostructures and the bottom metal film. Increasing the thickness of the dielectric spacer weakens the near-field coupling, causing the gap plasmon mode to degenerate into LSPR and FP resonance modes.

Miyata et al. designed a subwavelength color pixel structure based on an aluminum (Al) MIM plasmonic nanoantenna^[113]. As illustrated in Fig. 6(a) (1), the structure consists of a 100 nm thick Al film at the bottom, a 30 nm thick aluminum oxide (${\mathrm{Al}}_2{\mathrm{O}}_3$) dielectric layer in the middle, and Al nanocylinders (height 40 nm) at the top. The color strongly depends on the diameter of the nanocylinders, as depicted in Fig. 6(a) (2). They further combined nanostructures with different diameters into a unit cell to achieve a black subwavelength pixel. Using a single nanopillar, they demonstrated the printing of structural colors to form the word “Nano,” as shown in Fig. 6(a) (3).

Fig. 6

Designs based on plasmonic resonances in the gap plasmon. (a) Schematic of gap plasmonic structure based on aluminum nanorods (1), and achieving structural color pixels with a single nanostructure and black pixels by blending different nanostructures (2)^[113]. (b) Process flow and structural schematic of large-scale preparation of Ag nanorod gap plasmonic structures using colloid lithography, along with samples and characteristics in CMY mode—cyan, magenta, and yellow (2)^[114].

Blake et al. designed a subtractive color reflection structural color based on the gap plasmon mode^[114]. They utilized a hole-mask colloidal lithography (HCL) method to fabricate the top-layer nanodisk structures, achieving a large-area preparation process for reflective cyan, magenta, and yellow (CMY) structural colors, as illustrated in Fig. 6(b) (1). The self-assembly of colloids in HCL resulted in non-periodic distribution of Ag nanodisks as the top layer, a 30 nm thick ${\mathrm{Al}}_2{\mathrm{O}}_3$ spacer, and an Ag reflector as the bottom layer. Optimizing the structural parameters, they achieved vibrant and high-brightness reflective subtractive structural colors in cyan, magenta, and yellow. SEM images, reflection spectra, and CIE color coordinates are presented in Fig. 6(b) (2).

Overall, metal-plasmon-based structural colors have been a focal point of research in recent years, offering unique and vibrant coloration possibilities. In the pursuit of overcoming limitations associated with traditional pigments and dyes, researchers have explored the intricate interaction between metals and light. The use of metal nanostructures, such as gratings^[115,116], holes^[117], nanopillars^[118], etc.^[119–122] enables the manipulation of light through plasmonic effects. Structural colors based on metal plasmons can exhibit unparalleled performance, such as extremely high spatial resolution, excellent color stability, and simplicity in fabrication processes. Despite challenges related to brightness and color range, recent breakthroughs have addressed some of these issues, showcasing the potential of metal-plasmon-based structural colors in various applications, from display technologies to advanced optical encryption systems.

2.2.

Dielectric-Materials-Based structural color

Dielectric metasurfaces offer another method for generating highly saturated structural colors, but with much higher optical efficiency compared to their plasmonic counterparts^{[14,123–125]}. Dielectric materials inherently exhibit advantages over metals including high losses leading to broadened peak shapes and lower efficiency. However, dielectric materials cannot achieve the strong field localization of light that metallic nanostructures can, so dielectric nanostructures often require array-enhanced electromagnetic multilevel resonances, resulting in lower spatial resolution compared to metallic nanostructures.

Fundamentally, dielectric metasurfaces realize structural colors via Mie resonances, which depend on the geometric shape and size of particles^[126,127]. Multiple Mie resonances have been observed in various dielectric nanostructures, such as nanowires^[128,129], rings^[124,130], bricks^[131], cylinders^[123,132], and so on^[50,133,134]. The variety of available structures provides opportunities to modulate electric or magnetic resonances by designing specific geometric parameters. Apart from structural design, the physical properties of the material itself also significantly impact structural design.

Silicon (Si), as the most mature semiconductor material, has found widespread application in metasurface structural coloring. Si offers advantages such as low cost, high reliability, and compatibility with existing optoelectronic devices^[60,135]. Importantly, due to silicon’s high refractive index, it can effectively localize and manipulate the light field, leading to strong electromagnetic resonances when subwavelength-sized Si nanoparticles interact with visible light wavelengths. Therefore, Si nanostructures are well-suited for use as color filters to achieve structural colors with high purity and a wide color gamut. The results show that compared to metal-based structural colors, Si-based metasurfaces can achieve better color display effects^[136,137].

In 2020, Yang et al. designed a 100 nm thick single-crystal Si nanodisk structure on a sapphire substrate, as shown in Fig. 7(a)^[138]. To address background reflection and the wide resonance peak formed by Mie resonances, the authors introduced a refractive index matching layer to reduce the refractive index contrast at the air-substrate interface, effectively reducing background reflection and suppressing wide resonance modes. As shown in Fig. 7(a) (2), with the introduction of dimethyl sulfoxide (DMSO) as the refractive index matching layer, background reflection was significantly suppressed, simultaneously effectively inhibiting wide resonance modes and improving color monochromaticity. From the CIE chromaticity diagram plotted in Fig. 7(a) (3), it is clear that with the introduction of DMSO as the refractive index matching layer, the color gamut area expanded to 135.6% of Adobe RGB. Due to the high refractive index of single crystal Si, color display can be achieved with just a $2\times 2$ nanodisk array, allowing the final spatial resolution to exceed 100,000 PPI. This design achieves high reflectivity, narrow half height and width (FWHM), large color gamut area, extremely high spatial resolution, and a simple preparation process, taking a crucial step towards the practical application of dielectric structural colors.

Fig. 7

Structural color design based on Si. (a) Si nanorod array on a sapphire substrate, introducing PMMA and DMSO as refractive index matching layers for high-performance structural color (1), reflection spectra, and CIE coordinates of the sample (2), (3), displaying a vivid phoenix pattern (4)^[138]. (b) Preparation of different-sized air holes on Si surface, localizing the electric field in the air, achieving Mie resonance structural color at short wavelengths, with reflection spectra and electric field decomposition as hole size varies (1)–(3)^[139]. (c) Schematic of high-saturation red design based on Si nanoantenna array BIC mode (1), simulation and actual reflection spectra, and corresponding CIE coordinates (2), (3), (5), $Ez$ electric field components for both modes (4), and SEM image of the actual sample (6)^[140].

Due to the inherent strong absorption of Si at short wavelengths, which is unavoidable, and to address both the issue of absorption and material dispersion, Mario and colleagues proposed a strategy to confine light in subwavelength-sized air cavities^[139]. They successfully achieved Mie resonances based on a Si substrate, even in the blue and ultraviolet range. To demonstrate the nature of the resonance modes, the electric field distribution at the resonant wavelength is shown in Fig. 7(b) (2), revealing the presence of electric dipole and magnetic dipole modes within the air voids. By adjusting the pore diameter on the Si substrate from 300 to 750 nm and the depth from 20 to 1100 nm, nanoscale color printing covering the entire visible spectrum was achieved. The reflection spectra and optical microscope images are illustrated in Figs. 7(b) (1) and (3).

Despite significant progress in structural colors based on Mie resonances, achieving highly saturated red remained a challenge. High-saturation red requires fundamental resonances wavelength beyond 600 nm, but Mie resonances supporting red fundamental modes often also support high-order modes in the blue range (380 to 480 nm). This results in a shift towards blue, appearing as degraded magenta or purplish-red colors. To address this issue, Dong et al. introduced quasi-bound states in the continuum (quasi-BIC) modes as reflection modes for modulation in the field of structural colors^[140]. They supported two partially overlapping quasi-BIC modes on a Si nanoantenna array, simultaneously suppressing high-order modes in the blue/green range through the design of diffraction channels induced by the substrate and the absorption of amorphous Si. This achieved a highly saturated red structural color. The designed amorphous Si nanoantenna was optimized using a gradient optimization algorithm with structural parameters $L=235\mathrm{nm}$, $W=85\mathrm{nm}$, $\theta =47.9°$, $\mathrm{\Lambda }x=436\mathrm{nm}$, $\mathrm{\Lambda }y=432\mathrm{nm}$, $Hsi=360\mathrm{nm}$, as shown in Fig. 7(c). The simulated reflection spectrum in Fig. 7(c) (2) demonstrates distinct passbands and stopbands using quasi-BIC modes, closely resembling the spectrum required for an ideal Schrödinger red pixel. The actual measured reflection spectrum in Fig. 7(c) (3) aligns well with the simulation results. The CIE coordinates of the simulated and measured spectra are depicted in Fig. 7c (5). To verify the essence of the two response modes in the spectrum, Fig. 7(c) (4) shows the spatial distribution of $Ez$ at the corresponding wavelength of the reflection peaks. Optical microscope and SEM images of the actual sample are presented in Fig. 7(c) (6).

While Si has a high refractive index, its unavoidable absorption losses at short wavelengths result in low efficiency and reduced saturation due to the broadening of the bandwidth in visible range. To address the optical characteristics of the material itself, researchers have turned to dielectric materials with negligible losses in the visible light range, such as titanium dioxide (${\mathrm{TiO}}_2$)^[141–143], silicon nitride (${\mathrm{Si}}_3{\mathrm{N}}_4$)^[144–146], and so on^[51,147,148]. Among these, ${\mathrm{TiO}}_2$, with its excellent optical properties and compatibility with CMOS processes, has found extensive use in the field of optics^[149–151]. The efficiency and sharp resonance of ${\mathrm{TiO}}_2$ nanostructures supporting Mie resonances lead to high color saturation, easily surpassing the sRGB color gamut. However, due to the lower refractive index of ${\mathrm{TiO}}_2$ compared to Si, larger structural units and larger periodic arrays are required to enhance Mie resonances. In recent years, significant progress has been made in the study of metasurface structural colors based on ${\mathrm{TiO}}_2$.

Sun and collaborators demonstrated a Mie resonance structural color design based on an array of ${\mathrm{TiO}}_2$ nanoblocks^[134]. Figure 8(a) (1) shows a schematic of the proposed device, consisting of a trapezoidal-shaped array of ${\mathrm{TiO}}_2$ blocks on a glass substrate coated with 15 nm indium tin oxide (ITO). And the trapezoidal angles are approximately 72°. The manufacturing technique for this structure is achieved through a simple lift-off process. The fabricated structure closely matches the design dimensions, as shown in Fig. 8(a) (2). The simulated and measured reflection spectra in Fig. 8(a) (3) achieve high reflectivity of over 64% and FWHM of approximately 30 nm. However, when the fundamental mode resonance wavelength is in the longer wavelength range (580 nm), high-order resonance modes gradually appear in the blue range, leading to a decrease in color saturation. The CIE coordinates of sample colors with low color saturation obtained from the experiment are shown in Fig. 8(a) (4). This is due to the decrease in monochromaticity caused by higher-order modes and Mie multipole resonance at short wavelengths, resulting in an unsatisfactory final color display effect.

Fig. 8

Structural color design based on ${\mathrm{TiO}}_2$. (a) Design of trapezoidal ${\mathrm{TiO}}_2$ nanorod array structural color (1), (2), reflection spectra, and CIE coordinates for different sizes (3), (4)^[134]. (b) Schematic of structural color based on multi-layer dielectric nanorods (1), reflection spectra covering the entire color space (2), and Mie decomposition for any structure proving suppression of higher-order modes by multi-layer dielectric structures (3), (4)^[152].

To address the impact of high-order Mie resonance modes and Mie multipole resonance, Yang et al. designed a metasurface structural color using a multilayer dielectric stack to achieve deep modulation of Mie multipolar resonance modes, significantly enhancing the monochromaticity of the reflected spectrum^[152]. As shown in Fig. 8(b) (1), the designed metasurface structure consists of an array of nanoblocks on a Si substrate. Each nanoblock structure, from top to bottom, is composed of vertically stacked layers of a 100 nm thick silica capping layer, a 140 nm thick ${\mathrm{TiO}}_2$ spacer layer, and a 60 nm thick ${\mathrm{Si}}_3{\mathrm{N}}_4$ layer. The index matching between the ${\mathrm{SiO}}_2$ layer between ${\mathrm{TiO}}_2$ and air, and the ${\mathrm{Si}}_3{\mathrm{N}}_4$ layer between the silica substrate and the ${\mathrm{TiO}}_2$ layer, significantly suppresses the short-wavelength multipolar modes, as shown in Fig. 8(b) (3). Due to the deep modulation of multipolar modes, as shown in Fig. 8(b) (2), varying the structural parameters allows for achieving high reflectivity, high spatial resolution, low FWHM, and high saturation in a full color structural color.

Dielectric-metasurface-based structural colors represent a cutting-edge approach to coloration technology. By harnessing the unique properties of dielectric materials, researchers have developed metasurfaces with nanostructured patterns that manipulate light to create vivid and customizable colors. Compared with metal plasmon, dielectric metasurface structural colors offer superior brightness, a narrower resonant mode, and enhanced stability. Although dielectric materials tend to have lower resolution, dielectric metasurfaces are expected to drive the application of structural colors in various fields with their excellent properties.

4.1.

Phase Change Material

The addition of phase change materials to metasurfaces allows for reversible switching between different spectral responses through external stimuli. Vanadium dioxide (${\mathrm{VO}}_2$) has garnered attention due to its excellent thermal stability and reversible insulator-metal transition (IMT). In comparison to other materials, ${\mathrm{VO}}_2$ exhibits a relatively low IMT transition temperature ($\mathrm{T}=68°\mathrm{C}$) and faster transition speed (picosecond level)^[209,210], which has been used as thermochromic smart windows^[211]. He et al. designed a fully visible band switchable dynamically tunable absorber (DTA) based on ${\mathrm{VO}}_2$, with the proposed MIM structure shown in Fig. 11(a) (1)^[212]. The structure consists of a top layer of periodically perforated Ag, an intermediate layer of ${\mathrm{VO}}_2$, and a bottom layer of silver. By controlling the temperature of DTA to modulate the ${\mathrm{VO}}_2$ phase transition, a significant switching function is achieved across the entire visible light spectrum, as illustrated in Fig. 11(a) (2). This absorption change results in a noticeable color variation, depicted in Fig. 11(a) (3), showcasing the color change before and after the ${\mathrm{VO}}_2$ phase transition.

Fig. 11

Dynamic structural color design based on VO₂ and GST phase change materials. (a) VO₂ as a tunable dielectric spacer in MIM structure (1), and absorption and color changes before and after phase transition (2), (3)^[212]. (b) Dynamic structural color design based on GST, schematic of dynamic film and pixel tunable display structure (1), (2), structural colors with different film thicknesses (3), and schematic of flexible transparent display sample (4)^[215].

While ${\mathrm{VO}}_2$ exhibits excellent phase change performance, its phase transition process is volatile, hindering the preservation of color information in different states. ${\mathrm{Ge}}_2{\mathrm{Sb}}_2{\mathrm{Te}}_5$ (GST), as a mature phase change storage material, benefits from its significant optical performance change between crystalline and amorphous states. Its polymorphic adjustability allows for multilevel information storage^[213,214]. As early as 2014, research groups attempted to achieve dynamically tunable structural colors using GST material. In a study by Hosseini et al., a reflective display based on GST film was designed^[215]. The GST film is sandwiched between two layers of transparent ITO electrodes and deposited on the surface of a metal reflector, as shown in Fig. 11(b) (1). Color control is achieved by adjusting the thickness of each film layer, as illustrated in Fig. 11(b) (3). The GST pixels are pixelated, enabling an electrically switchable display where each pixel can be randomly accessed and manipulated, as depicted in Fig. 11(b) (2). By replacing the metal reflector on the back of the film with a transparent substrate, a semi-transparent display based on PCM can be realized. The structure is optimized from top to bottom with 20 nm thick ITO, 7 nm thick GST, and 40 nm thick ITO layers. Due to the thin thickness of the film, it can be deposited on flexible substrates, enabling a low power, ultrathin flexible display, as shown in Fig. 11(b) (4). Integrating PCM as an active switch for structural colors into the display makes ultrathin, low-power flexible displays possible.

However, GST’s relatively high optical losses in the visible light range make it challenging to achieve high-brightness structural colors. Another emerging PCM, antimony sulfide (${\mathrm{Sb}}_2{\mathrm{S}}_3$), has gained widespread attention due to its intense optical property changes, polymorphic adjustability during phase transitions, and lower optical losses in the visible light spectrum^[216]. Lu et al. utilized ${\mathrm{Sb}}_2{\mathrm{S}}_3$ to design a triple-resonance reversible and tunable dielectric nanodisk array, achieving nonvolatile, high-speed, and reversible tuning of Mie-resonance-based structural color devices^[217]. The ${\mathrm{Sb}}_2{\mathrm{S}}_3$ and Pd multilayered nanodisk array, arranged on a 200 nm thick ${\mathrm{SiO}}_2$ film on a Si substrate, is shown in Fig. 12(a) (1). The Pd layer, serving as the etching mask for ${\mathrm{Sb}}_2{\mathrm{S}}_3$ during inductively coupled plasma (ICP) etching, is deposited. Subsequently, a 70 nm ${\mathrm{Si}}_3{\mathrm{N}}_4$ layer is deposited to act as an anti-reflection coating, preventing the loss of sulfur (S) atoms during the phase transition process. Control over the ${\mathrm{Sb}}_2{\mathrm{S}}_3$ phase transition is achieved using a 780 nm, 80 MHz, 100 fs laser pulse, enabling a scanning speed of 10 µm/s at a power of 12 mW. The drastic refractive index change between the crystalline and amorphous states induces significant variations in the resonance modes, as observed in the reflection spectra in Fig. 12(a) (2). The multipole decomposition of the scattering cross-section is presented in Fig. 12(a) (3), illustrating the dynamic switching of structural colors as the ${\mathrm{Sb}}_2{\mathrm{S}}_3$ nanodisk transitions from the amorphous to crystalline state due to changes in the interaction between electric and magnetic dipole resonances.

Fig. 12

Dynamic structural color design based on Sb2S3. (a) Mie resonance structural model based on Sb2S3 nanorods (1), reflection spectra changes before and after phase transition (2), and Mie decomposition (3)^[217]. (b) Dynamic tunable FP resonance mode based on Sb2S3 (1), continuous color change achieved by controlling intermediate states of Sb2S3 phase transition, enabling multilevel adjustment of refractive index (2), (3)^[218].

Additionally, Omar et al. designed an all-optical switching structural color device based on ${\mathrm{Sb}}_2{\mathrm{S}}_3$^[218]. Figure 12(b) (1) illustrates the schematic of a multilayer film structure, where a 5 nm titanium (Ti) layer is first deposited to enhance the adhesion of Ag, followed by a 100 nm thick Ag layer serving as the back reflector. The dielectric portion consists of two layers of 25 nm thick ${\mathrm{Si}}_3{\mathrm{N}}_4$ (to separate the metal layer from the ${\mathrm{Sb}}_2{\mathrm{S}}_3$ layer) sandwiching a 100 nm thick layer of ${\mathrm{Sb}}_2{\mathrm{S}}_3$. Subsequently, a 10 nm Ti layer and a final protective layer of 10 nm ${\mathrm{Al}}_2{\mathrm{O}}_3$ are deposited. Control over multiple intermediate states of incomplete phase transition in ${\mathrm{Sb}}_2{\mathrm{S}}_3$ is achieved by controlling the continuous wave (CW) laser pulse density from 0 to $200\mathrm{kW}/{\mathrm{cm}}^2$ at a constant laser scan speed of 20 um/s, enabling switching between various refractive index states, as shown in Fig. 12(b) (2). Experimental validation demonstrates the multifunctionality of achieving various structural colors using the phase transition intermediate states in a single-layer ${\mathrm{Sb}}_2{\mathrm{S}}_3$ film within the MDM cavity. The transition from amorphous to fully crystalline state results in a resonance wavelength change of 220 nm, producing colors from green to red, as depicted in Fig. 12(b) (3).

4.2.

Liquid Crystal with Polarization Sensitive Metasurface

Unlike the phase change materials discussed earlier, which control optical responses by altering the material’s refractive index, the design of polarization-sensitive meta-atoms enables polarization-dependent optical responses. This approach allows color switching without changing the geometric shape or material composition. Numerous studies have explored polarization-dependent structural colors for applications such as dynamic color displays, high-density optical information storage, optical encryption, and multi-channel imaging^{[51,178,219,220]}.

Due to the optical anisotropy of liquid crystals (LCs), they exhibit different refractive indices in different directions, resulting in phase delays along different directions. Through the specific design of LCs, their ability to control polarization can be utilized. For instance, widely used LCDs rely on the control of polarization achieved by LCs. Recently, the development of tunable metasurfaces by combining LCs with metasurfaces has attracted much interest. For instance, researchers have integrated LCs with metasurfaces to create a device capable of dynamically displaying colors through voltage-controlled LC polarization modulation^[221]. In terms of commercial applications, liquid crystals are well-established commercial optical materials that have been extensively studied by many companies for the design of commercially available tunable metasurfaces, and exciting results have been achieved at telecommunication wavelengths^[222,223]. However, the combination of LCs and metasurfaces has not yet been successfully applied in commercial products for tuning structural color and remains in the laboratory stage.

Li et al. integrated a polarization-dependent plasmonic meta-surface with a polymer-dispersed liquid crystal (PDLC) as a polarization analyzer, achieving further encryption of transmitted light^[224]. The operational schematic of the device is depicted in Fig. 13(a) (1). By designing Al nanoapertures with different responses to x and y polarizations, the metasurface selectively displays images corresponding to specific polarization responses. Dynamic control of transmittance is achieved by applying voltage to the liquid crystal, with response and recovery times of 8.7 and 29.8 ms, respectively, under a 17 V voltage, as illustrated in Fig. 13(a) (2).

Fig. 13

Dynamic structural color adjustment using liquid crystal and polarization-sensitive metasurfaces. (a) Anisotropic Al nanoholes integrated with LC for switchable structural color display (1), and voltage-induced modulation of transmission intensity with a switch time on the order of milliseconds (2)^[224]. (b) Elliptical Mie resonators integrated with LC for brightness-adjustable dynamic color display (1), continuous changes in RGB color brightness under different polarizations (2), and dynamic color display of actual samples with increasing voltage (3)^[225].

Rho’s research team opted to integrate LC as a polarization generator with polarization-sensitive Mie resonators to achieve brightness-adjustable reflective structural colors, as illustrated in Fig. 13(b) (1)^[225]. The proposed Mie resonators consist of hydrogenated amorphous silicon (a-Si: H) ellipsoidal cylinders, arranged in a lattice with a specific periodicity. The desired spectral response is generated through the hybridization of Mie scattering with the periodic array’s quasi-guided mode resonance (qGMR). The spectral variations of the designed RGB primary colors with changing polarization are shown in Fig. 13(b) (2). Subsequently, LC is integrated as a polarization generator on the metasurface, enabling brightness control of colored patterns through voltage modulation, as depicted in Fig. 13(b) (3). By combining and arranging meta-atoms with different color responses, mixed colors can be generated, and combinations of red, green, and blue can produce white. The design based on polarization-sensitive and liquid crystal elements can find applications in various fields, including advanced optical encryption, optical anti-counterfeiting, multi-channel imaging, and dynamic displays.

4.3.

Mechanically Controlled structural color

Mechanically controlled metasurfaces were initially inspired by micro-electro-mechanical systems (MEMS), where temperature and voltage can be used to control micro-scale mechanical systems, thereby influencing the optical response of the combined metasurface at a microscopic level^[226,227]. Aaron et al. designed a voltage-controlled MEMS combined with a metasurface capable of selecting or mixing specific colors^[228]. The proposed structure uses silicon-on-insulator (SOI) technology to suspend Mie resonators on a Si substrate, as shown in Fig. 14(a) (1). The metasurface, composed of Si nanobeams (cross-sectional size $100\times 100\mathrm{nm}$), creates vibrant reflective structural colors through the coupling of Mie resonance and FP modes between the substrate and the metasurface. The driving capability of voltage for different thicknesses of Si metasurfaces was measured, as depicted in Fig. 14(a) (2). At a thickness of 100 nm, only 3 V of voltage was needed to drive over 100 nm displacement. By adjusting the voltage to control the height of the Mie resonator, dynamic tuning of the FP resonance wavelength was achieved, allowing the appearance of desired characters, as shown in Figs. 14(a) (3) and 14(a) (4).

Fig. 14

Dynamic structural color based on mechanical stress-induced structural changes. (a) Voltage-tunable FP resonance mode, adjusting grating structure height with changing voltage (1), (2), lowering height to induce resonance wavelength changes, and achieving color changes (3), (4)^[228]. (b) TiO₂ nanostructure array prepared on a flexible substrate (1), and dynamic adjustment of structural color by applying external stress (2)^[229]. (c) Kirigami grating structure prepared via nanoimprinting and laser etching (1), grating structure exhibiting strong selectivity for observation angle (2), and dynamic structural color display achieved by applying external force or combining with a drive motor (3), (4)^[230]. (d) Composite of ATO nanoparticles and mechanically responsive color-changing pigment in a highly elastic liquid crystal substrate (1), achieving dynamic color changes with high saturation and a wide color gamut (2), (3)^[231].

While dynamic structural colors based on MEMS have achieved significant progress, the complex composition of MEMS structures and their integration with metasurfaces pose significant challenges in terms of processing and design, greatly limiting the effective application of structural color devices. However, stress-induced modulation based on a flexible substrate is a simple and effective control method. Zhang et al. investigated the dynamic tuning of ${\mathrm{TiO}}_2$ metasurface structural colors through PDMS stretching, achieving polarization insensitivity in two independent mechanisms parallel and perpendicular to the stretching direction, as illustrated in Fig. 14(b) (1)^[229]. The metasurface is presented as an inverse trapezoidal ${\mathrm{TiO}}_2$ nanostructure array embedded in a PDMS flexible substrate. Through the analysis of the scattering cross-section’s multipole decomposition, clever adjustments to the structural parameters enable the movement of resonance positions based on deformation under different polarization states, allowing for information display and concealment, as shown in Fig. 14(b) (2).

Inspired by the structural color changes caused by the movement of animal feathers, Hou et al. designed a structure that utilizes topological spatial deformation on a two-dimensional (2D) plane with a kirigami structure to manipulate the direction of a 1D grating^[230]. The topological deformation generated by stretching allows for predictable and precise adjustment of pixelated grating direction, enabling controlled changes in structural color. The gratings, made of PDMS flexible material, were mass-produced using nanoimprint technology, and pixelated gratings were cut using laser cutting, as shown in Fig. 14(c) (1). Figure 14(c) (2) demonstrates that vibrant structural colors can only be observed at an observation azimuth angle of 90°. The essential nature of topological deformation induced by external stress is changing the orientation of grating pixel blocks. Selective stretching of the kirigami grating can achieve independent control of each segment, as depicted in Fig. 14(c) (3). It can also be combined with a dielectric elastomer actuator drive to achieve voltage-driven dynamic structural colors, as shown in Fig. 14(c) (4).

In a different approach, inspired by the color-changing ability of cephalopod skin^[232], Sun and collaborators proposed a biomimetic liquid crystal elastomer film (BLCE) based on force-induced coordinated changes in pigment and structural colors^[231]. Control over mechanical sensitivity was achieved by adjusting the concentration of antimony-doped tin oxide (ATO) nanoparticles, as illustrated in Fig. 14(d) (1). When the critical elongation rate for the pigment is not reached, the color is primarily caused by the structural color resulting from changes in the spacing of the liquid crystal elastomer helix. After exceeding the critical elongation rate, the color exhibits a combined effect of structural and pigment colors, achieving continuous dynamic color changes from red to blue at elongation rates from 0% to 100%, as shown in Figs. 14(d) (2) and 14(d) (3). Combining force-induced pigments and structural colors, the design of BLCE film effectively addresses the issues of low elongation rate and small viewing angle of PDMS substrates. Due to its outstanding force-induced response and a sufficiently large color display range, BLCE films hold great potential in applications such as mechanical sensors and anti-counterfeiting materials.

5.1.

Display Technology

With pixel densities, brightness, and color saturation surpassing current displays by two orders of magnitude, structural colors are being recognized by numerous researchers as formidable contenders for the next generation of high-performance displays^[236,237]. Substantial research efforts have been dedicated to structural color displays to harness their superior capabilities. To achieve in-situ dynamically reconfigurable structural color displays, Yan et al. devised a floating solid thin film (FSTF), as illustrated in Fig. 15(a) (1)^[188]. The film, consisting of a 45 nm thick ITO layer, a 70 nm thick iron oxide layer, a 140 nm thick Ag layer, and a 100 nm thick TiW layer, undergoes reconfiguration by applying bias voltages to the ITO and TiW electrodes, thereby driving the movement of Ag ions. The cross-sectional SEM of the FSTF sample is depicted in Fig. 15(a) (2). Without bias, the resonant wavelength can be controlled by adjusting the thickness of the ${\mathrm{Fa}}_2{\mathrm{O}}_3$ layer, as shown in Fig. 15(a) (3). As illustrated in Fig. 15(a) (4), choosing a 70 nm ${\mathrm{Fa}}_2{\mathrm{O}}_3$ layer, and applying a 1 V positive bias to the electrode, results in a color transition from orange to purple, blue, and green over time. Reversing the process with a 1.3 V inverse bias enables reversible changes in structural color. Each color state is non-volatile, exhibiting long-term optical stability. Subsequently, flexible FSTF films were prepared on a flexible substrate, displaying a wide viewing angle and polarization insensitive characteristics, making them highly suitable for flexible display technologies.

Fig. 15

Applications of structural color in the display. (a) Voltage-driven in-situ color-changing multilayer film structure (1), (2), initial colors of different thicknesses of ${\mathrm{Fe}}_2{\mathrm{O}}_3$ layers (3), and reversible color changes under positive and negative bias (4)^[188]. (b) High-resolution OLED design based on structural color surfaces (1), controlling FP mode by adjusting OLED layer thickness (2), achieving higher brightness at the same power due to reduced optical losses of traditional color filters, and maintaining good color display even with a minimum subpixel structure of 1.2 µm (3), (4)^[238]. (c) Combining color filters with micro lenses to achieve 3D structural color display is illustrated. Schematic diagram of 3D display achieved through diffuse light (1). SEM images of the display unit and a 3 pixel × 3 pixel unit, where each pixel consists of $5\times 5$ nanopillars (2)^[241].

Joo et al. designed a metasurface-based OLED display screen serving as a coordinated back reflector, achieving an ultra-high resolution of over 10,000 PPI^[238]. The structure of the meta-OLED device is depicted in Fig. 15(b) (1), where an Ag nanopillar array is constructed on the Ag reflector, and OLED structures for RGB emitters and charge transport layers are built on the metasurface. Figure 15(b) (2) illustrates the color representation of nanopillars with different structural parameters, with the background color determined by the OLED layer’s thickness. This outcome indicates that a judicious combination of OLED and metasurface allows for achieving any desired color in the visible spectrum. Due to the increased design flexibility provided by the metasurface for OLEDs, coupled with the Purcell effect, the meta-OLED exhibits superior emission performance and a shorter spectrum compared to color-filtered white OLEDs, as shown in Fig. 15(b) (3). Accurate color display and high brightness standards are maintained even at a sub-pixel size of 1.2 µm, achieving a pixel density of 10,000 PPI, as illustrated in Fig. 15(b) (4). The OLED design based on metasurface structural colors is poised to be a formidable contender for the next generation of micro displays, boasting high saturation, brightness, and exceptional spatial resolution, making it one of the most practical applications of metasurface structural colors.

Different from traditionally applying structural colors to 2D flat displays, Joel and colleagues employed a 3D display technology proposed by Nobel laureate Gabriel Lippmann^[239,240]. They combined structural color planes with a micro-lens system, achieving 3D structural color displays observable to the naked eye under diffused light, as illustrated in Fig. 15(c) (1)^[241]. To achieve a seamless integration of micro-lenses and structural colors, a two-photon polymerization 3D printing technique was employed to simultaneously print nanopillars and micro-lenses. The micro-lens had a curvature radius (R) of 22 µm and a diameter (L) of 21 µm. The positions of the micro-lenses and the arrangement of nanopillars were determined through ray-tracing calculations. The actual structure is depicted in Fig. 15(c) (2).

5.2.

Optical Multi-Regulation

Due to the multidimensional control of light achieved by metasurfaces, unique responses to different states of light can be realized through the unique design of metasurface units^[242]. Exploiting this capability, structural colors find widespread applications in optical multi-states information regulation. Typically, utilizing the anisotropy of meta-atoms to achieve different colors for various polarization states is the most common optical encryption method^[243–247]. Alternatively, multiple colors can be further encoded using encryption techniques such as binary or Morse code^[86,248,249]. However, achieving foolproof advanced optical encryption with these methods can be challenging. To achieve a higher level of optical encryption, Joel’s research group combines structural colors with OAM^[250]. By associating different orders of OAM with colors, optical information is stored in the form of OAM and color. The information is decrypted using a physical key, enhancing optical security. To improve the signal-to-noise ratio, they introduce a converging phase in the color-topological vortex beam (CVB). The actual CVB sample is depicted in Fig. 16(a) (1). Since color and topological charge are independent, a single CVB array can be used for multidimensional information storage and optical anti-counterfeiting, as shown in Fig. 16(a) (2). In a single CVB array, the color displays the information “SUTD,” while the topological charge shows mathematical information, allowing independent control of any piece of information. The decryption process, based on a physical key and colored vortex beams, is illustrated in Fig. 16(a) (3). Photon key A consists of a $3\times 3$ array of CVB units. White light passing through A is then encoded with different information-carrying vortex-colored beams, enabling decryption of color, OAM, and spatial information.

Fig. 16

Applications of structural color in optical encryption. (a) Advanced optical encryption design combining orbital angular momentum (OAM). SEM image of a single CVB unit (1). Individual control of color and OAM information on a single surface (2). Optical decryption process based on physical keys (3)^[250]. (b) Laser-induced volcano-like nanostructures on MIM surfaces (1), volcano structures showing significant angular anisotropy (2), precise control of nanostructure size by adjusting laser power (3), and utilizing volcano-like nanostructures for advanced optical steganography (4)^[251].

On the other hand, planar optical devices based on nanostructures are crucial for implementing optical steganography. Hu et al. designed a volcano-shaped plasma structure using femtosecond laser printing and demonstrated its application in angle-dependent hidden color images^[251]. The schematic diagram of angle-dependent steganography is illustrated in Fig. 16(b) (1). On an MIM structure composed of a 40 nm thick Ti layer, a 126 nm ${\mathrm{Si}}_3{\mathrm{N}}_4$ dielectric layer, and an 80 nm thick Ag layer, fs laser pulses were used to irradiate the Ti layer, allowing precise control of laser power to print volcano-shaped nanostructures of different morphologies and heights on the MIM surface, as shown in Fig. 16(b) (3). Structures of different morphologies and heights exhibit angle-dependent structural colors, as depicted in Fig. 16(b) (2). This characteristic is exploited to achieve angle-dependent image steganography, as shown in Fig. 16(b) (4), where the sample displays different colors and information at incident angles of 27° and 52°.

Owing to the strong control of light at subwavelength scales, metasurfaces have been extensively researched for their multidimensional optical modulation capabilities. Through the unique design of metasurface units, researchers have achieved multiple functionalities on a single metasurface. Among these functionalities, the realization of two-dimensional or three-dimensional holographic image reconstruction through phase modulation has garnered significant attention in display technology^[252–254]. To extend the applications to areas such as advanced optical encryption and higher-density optical information storage, it becomes crucial to simultaneously modulate spatial phase and spectral response within a single-layer metasurface^[255–261].

Kim et al. proposed an advanced encryption metasurface that combines structural colors and vector holography^[262]. In this design, the metasurface unit serves as both a Mie resonator to generate structural colors and a local half-wave plate for phase control. The control of Mie resonance is determined by the geometric parameters of the nanopillars, and the phase is achieved through geometric phase, only related to the rotation angle of the nanopillars. Therefore, it is possible to simultaneously design a single metasurface device that incorporates color, amplitude, and phase information, as shown in Fig. 17(a) (1). Nine different phase control units were designed based on the incident left- or right-circularly polarized (LCP or RCP) light, and these units were constructed into a metapixel to generate nine polarization states, as shown in Fig. 17(a) (2). To simplify the control of holographic polarization information, LC units were integrated into the metasurface. By applying voltage to the LC units, switching between different phase gradient holographic information displays could be achieved, as shown in Fig. 17(a) (3). This design can be used as an optical encryption anti-counterfeiting label, using structural color as the primary encryption and holographic images as the secondary encryption, thereby realizing a more advanced optical anti-counterfeiting process.

Fig. 17

Applications of structural color in the field of multiple information. (a) Metasurface enabling both structural color and holographic display of multiple information (1), multiple nanostructures forming a unit cell, modulation of holographic image information through integrated LC (2), and combining structural color with voltage-driven holographic images for multiple information transfer and advanced optical encryption (3)^[262]. (b) 3D integrated metasurface for high-performance multifunctional displays. Metasurface structure shiyitu1 and SEM image (1). Simulation design and actual structural color with holographic images (2)^[263].

Unlike conventional methods that simultaneously control amplitude and phase through a single surface, Hu et al. designed a three-dimensional integrated metasurface^[263]. They integrated dielectric nanohole structures for phase modulation on a Fabry-Perot (FP)-cavity-based filter, allowing for separate modulation of amplitude and phase. This design provides more degrees of freedom, enabling features like low crosstalk, high efficiency, and simple configuration. The schematic of the three-dimensional integrated metasurface is shown in Fig. 17(b) (1). The structural color part is composed of an Ag/HSQ/Ag FP cavity on a quartz substrate. The 150 nm thick HSQ serves as the spacer layer between the filter and the phase plate, with phase modulation achieved through PMMA hole structures. Different-colored FP cavity structures can serve as different color channels. By combining grayscale monochromatic images from RGB channels, a full-color holographic image can be obtained, as illustrated in Fig. 17(b) (2).

5.3.

Coating or Ink

In everyday life, the extensive use of dyes is commonplace. Traditional chemical pigment synthesis often struggles to produce colors that are vibrant and bright enough, and it is plagued by issues of fading. Moreover, the synthesis process is associated with environmental concerns related to pollution and recycling. The use of structural colors as a replacement for traditional pigments in daily applications, such as color coatings and ink printing, has long been a major goal in the field of structural colors^[264–268].

Demirörs et al. designed an isotropic structural color generated by photonic colloidal glass^[269]. The colloidal ink used for printing is a copolymer formed by ${\mathrm{SiO}}_2$ nanoparticles, carbon black, and gel. Carbon black serves as an absorbing medium to reduce multiple scattering, while the gel controls the rheological behavior of the ink. These inks can achieve both the 3D shaping of colloidal glass and self-assembly. The printing process is illustrated in Fig. 18(a) (1). After printing the structure, heating is applied to remove the liquid phase and gel from the ink, resulting in the formation of colloidal glass and the generation of isotropic structural colors. The color can be adjusted by changing the size of the ${\mathrm{SiO}}_2$ particles in the ink, as shown in Fig. 18(a) (2). This ink design can be adapted for different printing devices by adjusting the volume fraction of the nanoparticles. Furthermore, the structural color ink employs nontoxic and sustainable components, addressing pollution issues associated with traditional chemical dyes.

Fig. 18

Applications of structural color in coatings and ink fields. (a) Preparation of ink with mixed silica nanoparticles for printing, removing excess liquid phase by heat treatment (1), and easy adjustment of ink color by changing nanoparticle diameter (2)^[269]. (b) Self-assembled Al nanoparticles on alumina surfaces for creating plasmas used in the preparation of super-light coatings (1), due to the isotropic nature of self-assembled particles, exhibiting polarization- and angle-insensitive properties (2), controlling color by adjusting the deposition time of Al atoms (3), and preparation of super-light coatings with only 0.4 g/m² in organic solvents (4)^[87].

To enhance the practicality of structural colors in the field of coatings, it is necessary to design nanostructures that are insensitive to polarization and achieve a large viewing angle. Figure 18(b) illustrates a structural design based on gap plasmons to achieve polarization and angle insensitivity^[87]. As depicted in Fig. 18(b) (1), an absorption layer consisting of self-assembled Al nanoparticles, a dielectric layer, and an Al back mirror collectively generates colors in a subwavelength resonant cavity. At sufficiently low electron beam evaporation rates, Al atoms self-assemble on the oxide substrate, forming small clusters of nanoparticles. The size of the nano islands can be controlled by adjusting the deposition time. Therefore, this self-assembly property can be utilized to achieve large-scale structural color fabrication using a deposition-only process. Fig. 18(b) (2) demonstrates the color display capability of the sample with polarization and angle insensitivity. Since this structure achieves structural colors through a subtractive color scheme, a single-layer structure cannot produce green. Therefore, green is achieved by using multiple layers of Al plasmons, resulting in the final color distribution as shown in Fig. 18(b) (3). Additionally, the authors created independent bidirectional color flakes on both sides of the Al back mirror and crushed them to produce powder, which can be stored in air or organic solvents, forming a structural color coating, as shown in Fig. 18(b) (4). Due to the thickness of the coating being maintained at the level of 100 nm, it can reach an astonishing $0.4\mathrm{g}/{\mathrm{m}}^2$. While being hundreds of times lighter than traditional pigments, it can provide a more environmentally friendly and stable color display.

5.4.

Sensor

The dynamic and reversible control achievable by externally modulating the nanostructures responsible for structural colors makes them sensitive to external stimuli. This characteristic has led to the application of structural colors in sensing, with extensive research focusing on applications such as motion sensing^[270], tensile and shear stress sensing^[271,272], passive humidity sensing^[273–275], gas sensing^[196,276], refractive index sensing^[277], PH sensing^[278], spectrometers^[279,280], and temperature sensing^[85,181,212]. In contrast to physical and chemical sensing, biological sensing often involves complex processes, lengthy detection times, and challenges in achieving real-time monitoring. The real-time color changes exhibited by structural colors in response to biological samples significantly reduce the complexity and time of biological detection, enabling easy implementation of real-time monitoring. Structure-color-based biosensors have been widely researched and commercialized due to these advantages^[281–285].

Metal SPP modes can generate vivid structural colors, and the resonances of localized surface plasmons exhibit sensitivity to changes in the refractive index of the surrounding environment. Therefore, SPP-based structural colors are widely researched in areas such as biological imaging and biochemical analysis^[286–288]. In the field of biology, traditional cell staining methods allow observation of different parts of cells by staining, but this process inevitably damages the cells. Therefore, achieving non-destructive observation of the living state and internal conditions of active cells has been a longstanding challenge. Brian’s research team designed a patterned array of Ag nanoholes, referred to as “nanoslides,” and introduced them into a cell microscopy system, enabling non-destructive color observation of live cell slices under an optical system^[289]. The biological microscopy slice model based on nanoslides is depicted in Fig. 19(a) (1). Nanoslides consist of an Ag nanohole array covered with a protective layer of approximately 10 nm thick ${\mathrm{SiO}}_2$. As the SPP modes are highly sensitive to changes in the dielectric constant, different regions of the biological slice cause varying degrees of redshift in the SPP mode wavelength, resulting in distinct color changes. To test the optical contrast of nanoslides, Pt/C with thicknesses of 3, 8, 13, and 19 nm was deposited on the SPP sample surface for testing. As illustrated in Fig. 19(a) (2), nanoslides exhibited a resolution sensitivity exceeding 3 nm. The ability to determine the dielectric constant of materials based on color changes was also validated by the authors. When applied to the observation of human epithelial cell slices, cancerous cell tissues exhibited significantly different color responses compared to normal cell tissues. This design holds promise for further applications in rapid pathological detection of certain diseases.

Fig. 19

Applications of structural color in the field of biosensors. (a) Cellular color observation based on structural color of metal metasurfaces. Biological slice model based on nanoslides, and two different designs of metasurface models (1). Testing with nanoslides for different thicknesses of Pt/C, showing significant color differences for 3, 8, 13, and 19 nm, achieving a resolution of over 3 nm (2)^[289]. (b) Plasmonic structure based on M13 bacteriophage as a biological medium for lung cancer detection (1), validation of color array for quantitative and qualitative analysis of different organic compounds (2), and combining DNN training to achieve 90% accuracy in disease diagnosis (3)^[290].

On another note, structural colors have garnered widespread attention in the field of biosensing due to their distinct color changes, low sample requirements, rapidity, and being visualizable, among other advantages. Nguyen et al. developed a controllable gap plasmon color film (GPCF) by combining metal nanostructures with M13 bacteriophage for the detection of volatile organic compounds (VOCs), aiming at diagnosing lung cancer through color changes in the sensor^[290]. As illustrated in Fig. 19(b) (1), the M13 bacteriophage layer acts as a modulator placed between the Ag reflector and Ag nano-cube structure. By using M13 bacteriophages modified with four different proteins and different biological layers with thicknesses of 20, 30, and 40 nm for each, a colorimetric array based on plasmonic color films was designed. The GPCF was tested for its response to various organic compounds and their concentrations, revealing a unique response to different organic molecules and concentrations. Thus, through result analysis, it can achieve identification and concentration determination of individual gases, enabling quantitative analysis as shown in Fig. 19(b) (2). Furthermore, by using the structural colors resulting from the interaction of breath gases from lung cancer patients with the colorimetric array as training samples for a convolutional neural network (CNN), the CNN model achieved discrimination between lung cancer patients and healthy participants with accuracies of 90% and 92.8%, as illustrated in Fig. 19(b) (3). GPCF enables rapid preliminary detection of diseases, providing a relatively fast and accurate health monitoring sensor for real-time monitoring. However, biomedical monitoring often requires higher precision, and existing SPP-based biosensors still struggle to meet the high-precision quantitative analysis required for practical medical applications. In pursuit of higher detection accuracy, more sensitive optical modes, such as continuum-bound states, can be employed. Altug and colleagues established an outstanding and versatile sensing platform using BIC modes in the near-infrared wavelength range^[291]. However, further research and design are still needed for the application of visualizing BIC-based biosensing in the visible light spectrum.