etc. In order to maximize the utilization of solar energy, STPV requires the cooperative spectral manipulation of a broadband solar absorber and a narrowband infrared emitter. An ideal STPV absorber must simultaneously absorb input power and suppress radiation loss, while an STPV emitter should possess high emissivity only at the target infrared wavelength matching well with the base PV cell. [9] Extensive efforts have been devoted to design and fabricate such absorbers and emitters, including intrinsically spectrally selective materials, [10][11][12] multilayer structures, [13][14][15][16][17] cermets, [18] plasmonic metamaterials, [19][20][21][22][23][24][25][26] and photonic crystals. [27][28][29][30][31] Up to now, most of the reported absorbers and emitters are demonstrated by two isolated structures, [1,2] such as the compound metallic structures patterned on both sides of a substrate in a recently developed STPV system. [30] Such an optical design is intuitive and straightforward. However, the double-side lithography process severely increases the fabrication and systematic complexity. A hybrid absorber-emitter (HAE) with the two functions built on the same surface of the structure is beneficial for STPV. Great efforts have been made to integrate these two functionalities of broadband-absorption and narrowband-emission into one metasurface or plasmonic structure. [32][33][34] However, these structures are rather complicated and the well-defined morphologies are unstable at high temperature that the STPV system requires. An integrated HAE with ideal spectral selectivity, high temperature tolerance as well as scalable fabrication process is highly pursued but still elusive.Most specifically, in this work, we present a much simpler HAE design of a layered structure on a metallic surface based on multiple coherence-enhanced absorption, especially the coherent perfect absorption (CPA) effect. Such a structure is lithography-free, scalable, and possesses excellent thermal stability. In addition, the full spectrum responses demonstrate weak angular-dependence and polarization sensitivity, all of which make it beneficial for the STPV applications.The CPA phenomenon was first proposed for the case that two coherent counter-propagating light beams can be totally absorbed in a dielectric Fabry-Pérot cavity, [35][36][37] which was Spectrum selective absorbers and emitters, with advantages of high temperature tolerance, wide angle insensitivity, and scalable fabrication processes, are crucial components for solar thermophotovoltaics (STPV). A bifunctional hybrid absorber-emitter (HAE) for efficient STPV by sequentially depositing HfO 2 /Mo/HfO 2 films on a metallic surface is demonstrated here. Simultaneous broadband solar absorption and narrowband infrared emission are enabled by the same surface of the structure. By fine steering coherent perfect absorption of the ultrathin Mo film and destructive interference of interfacial reflections across the top HfO 2 layer, the HAE exhibits a measured emissivity of 0.97 at 1.8...