COMMUNICATIONDue to its advantage and promising applications, many recent studies have been focused on the design of F-P cavities-based spectral fi lters. [ 35,36 ] For example, Aydin and coworkers proposed a perfect absorber comprised of planar Ag/SiO 2 /Ag cavity with a maximum absorption intensity of ≈97% and a narrow bandwidth of ≈17 nm. [ 37 ] Furthermore, the location of the absorption peak is tunable in the visible light range just by controlling the dielectric spacer thickness. Yang et al. obtained three primary RGB (red, green, and blue) refl ective colors with a low sensitivity to the incidence angle by fabricating asymmetrical resonant cavities comprised of an a-Si dielectric fi lm sandwiched by a thin chromium (Cr) layer and a thick silver (Ag) layer. [ 38 ] In their structure, Cr is adopted as the absorptive layer to absorb the incident light and the RGB fi lters are achieved by adjusting the thickness of the constituent layers. However, it is noteworthy that the purity and brightness of the existing proposed color fi lters to date are not suffi ciently high due to the narrow absorption peak and the relatively low refl ectivity in the wavelength range of the color we are interested in.In this work, F-P cavities-based refl ective color fi lters consisting of a layer of thin nickel (Ni) fi lm and a thick aluminum (Al) fi lm, separated by a silicon dioxide (SiO 2 ) dielectric layer, are demonstrated. We use a thin nickel (Ni) layer as a broadband absorber to obtain abundant structural colors with high saturation and brightness operating at visible range. Combined with grayscale patterning techniques, we also demonstrated that high-resolution, high-contrast monolithic color printing could be achieved enabled by this refl ective color-fi lter confi guration.The schematic confi guration of the proposed refl ective color fi lter is shown in Figure 1 a. It is an asymmetric F-P type resonator comprised of Ni/SiO 2 /Al triple-layer fi lm stacks, in which the refl ectivity of Ni and Al is very different. Ni was chosen to be the top metal because of its relatively uniform and appropriate refl ectivity and absorption in the entire visible light range which is essential to achieve broadband absorption for purer and brighter refl ective colors, as indicated by the simulated refl ectance and transmittance spectra in Figure 1 b. Al was adopted as a highly refl ective mirror at the bottom. SiO 2 is a lossless dielectric material in the visible range, which was used as the spacer layer, and its optical thickness d determines the position of the absorption and refl ectance peaks. Comparing to other designs using Ag as absorber and mirror, both Ni and Al in the confi guration have better adhesion property with SiO 2 and are also inexpensive for practical applications.Metal-based refl ective color fi lters, which display various colors by selectively refl ecting a specifi c wavelength in the visible region, have attracted tremendous interest in recent years as a crucial component for diverse applications, such as optical ...