in balancing out optimum thicknesses for charge extraction and efficient light absorption. [6] The ultimate goal of a lighttrapping strategy is to achieve complete absorption of light in a broad spectral range while using the minimum amount of photoactive material. Traditional waferbased technologies have extensively exploited light-trapping strategies up to a point where the classical limit of light trapping [7,8] is almost reached. [9] There is, however, an increasing interest in further decreasing the thickness of the active layer below the micron, where new properties appear for classic materials (such as flexibility for silicon [10] ) and new materials like plastics [11] or nanocrystals [12,13] can be used at lower processing costs. Capturing light in such ultrathin devices requires redesigning the strategy, moving away from traditional ray optics approximations into the wave optics regime. [6] Many wave optics based designs are being currently investigated; photonic crystals (PhCs), [14,15] plasmonics, [16,17] and microresonators [18][19][20] provide new and exciting means of confining light in subwavelength thin films. Nevertheless, strong absorption enhancements are not restricted exclusively to the above-mentioned photonic architectures. Kats et al. [21] demonstrated flat nanometric films (up to 25 nm) of amorphous germanium (a-Ge) with 90% absorption in the visible range when deposited on optically thick gold films. Simply put, nanometric semiconductor coatings on metallic films act as Gires-Tournois interferometers [22,23] (a Fabry-Perot resonator where one of the interfaces is metallic). Such absorption comes from a strong interference effect originated by both the nonideal behavior of the metal film at visible frequencies (allowing field penetration in the metal) and the high values of the complex refractive index of the semiconductor. In-depth analysis of these results revealed that this system sustains Fabry-Perot resonances (FPRs) coupled with Brewster modes, [24] which are incident wave modes with no scattered wave that can be accessed from air. The excitation of this Brewster mode is possible at normal incidence and endows the system with omnidirectional strong absorption [25] (Figures S1 and S2, Supporting Information). The thickness of the semiconductor layer determines the position of the minimum in the reflectivity (maximum in absorption) of these resonances with the particularity that, because of the penetration depth in the metal, the resonant condition is below the classical λ/4 condition. SuchThe design of ultrathin semiconducting materials that achieve broadband absorption is a long-sought-after goal of crucial importance for optoelectronic applications. To date, attempts to tackle this problem consisted either of the use of strong-but narrowband-or broader-but moderate-light-trapping mechanisms. Here, a strategy that achieves broadband optimal absorption in arbitrarily thin semiconductor materials for all energies above their bandgap is presented. This stems from the strong interplay...