In recent years, metamaterials have become a research hotspot and achieved significant progress in both military and civilian applications due to their great potential in control of amplitude, phase, and polarization of electromagnetic (EM) waves. It can be potentially applied in stealth technology, photonics, and wireless communications. [1][2][3][4][5][6][7][8][9][10][11] Metamaterial absorbers (MAs), the specialized functional devices for capturing and dissipating EM waves, have attracted extensive attention due to their wide range of applications in energy harvesting, EM compatibility, stealth technology, and sensors. [12][13][14][15][16][17][18] Since the first attempt with perfect absorption realized based on metamaterials, [19] the interested operation range of MAs has been extensively expanded from microwave, terahertz (THz), and infrared to visible light. [16][17][18][19][20][21][22][23][24] Nevertheless, the early attempt suffers from a series of drawbacks, such as narrowband, and polarizationand angle-sensitive performance, which significantly limit their real-world applications. To solve the earlier issues, researchers have developed several strategies to achieve absorbers with multiband, broadband, wide-angle, polarization-insensitive, and even tunable characteristics. [25][26][27][28][29][30][31][32][33][34][35][36] For example, fractal structure was involved in a tripleband absorber design, leading to multiple local resonant circuits and thus contributing to near-unity absorption for a wide range of incident angles under dual-polarization states. [31] To date, several approaches have been proposed to widen the operating bandwidth, including creating multiple resonances by introducing planar/vertical inclusions, [32][33][34][35][36] and lumped elements such as resistances, capacitances, and diodes. [37][38][39][40][41][42] However, there are still some issues remaining unaddressed. For planar structures with single-layer composite patterns, the design is extremely complicated, and the expansion of bandwidth is often limited. Moreover, previous multilayer absorbers always feature bulky and much larger volumes than the theoretical limit established by Rozanov for physically realizable absorbers. [43] As for the lumped approach, it is impossible for high-frequency operation or elegant miniaturization and leads to even more complexity. The advent of indium tin oxide (ITO) film provides an efficient solution to the earlier issues due to its resistance characteristics and wide commercial availability. Although most of absorbers based on ITO can achieve broad bandwidth by combining the approaches of introducing resistances and multilayer patterns with air spacer, they increase considerably the thickness of the absorber. [44][45][46][47][48] At present, it is still a great challenge to obtain broadband absorbers with a low profile that are desirable in specific applications.Here, we propose a multimode-assisted strategy to acquire a trilayer broadband MA with simple patterned ITO films in a