are the most commonly used methods to resolve above trouble. Although many good results [18][19][20] have been extensively achieved, the limited maneuverability of the material para meters and the complexity of the synthesis process still restrict their practical application. The recent development of metamaterial absorbers based on subwavelength thickness structures has injected new impetus into this subject. Compared with traditional absorbing materials, metamaterials show the advantages of tunability, thin thickness, and lightweight, with simple geometry for both experimental implementation and mass production. Moreover, metamaterial absorbers can exhibit near-unity absorption at a certain frequency or several discrete frequencies due to both their inherent resonance mechanism and the accompanying dispersion. [21][22][23] Considering the broadband absorption advantage of traditional microwave absorbing materials in high frequency region and the flexible adjustability of electromagnetic (EM) parameters of metamaterials, the combination of metamaterials and traditional absorbers will give play to their respective advantages, which is a more ideal way to obtain high-performance absorbers. For example, the cruciform meta-atom is periodically arranged and embedded into carbonyl iron particle (CIP) coating, enhancing the average reflection loss by 45.8%. [24] When a metamaterial as an intermediate layer is inserted between two magnetic coatings, multiple resonances will be introduced to effectively broaden the absorption bandwidth. [25,26] These methods focus more on the ability of metamaterials to dissipate EM waves but ignore the wavefront modulation of metamaterials, which also can extend EM absorption spectrum. Guan combined a nonplanar magnetic metamaterial and a magnetic coating into a hybrid absorber, exhibiting 90% absorptivity around 2.4 GHz and over the 8-18 GHz. [13] Liang proposed gradient impedance metamaterial as impedance matching layer and combined it with multilayer ITO metamaterial to realize ultrawideband absorption at 1-18 GHz. [27] Regretfully, the total thickness of above configurations both exceed 10 mm, and the latter even reaches 31.6 mm. Obviously, these non-systematic conceptual-based designs with large lattice constants lead to a large thickness, which is not acceptable for the MAMs. Even so, metamaterials can be used as impedance matching layer to induce EM waves into magnetic coatings to promote Despite great efforts in material design and modification, there are still obstacles to improve the effective microwave absorption, which hinders the development of stealth materials. By introducing a magnetically induced Huygens' metasurface with Fibonacci spiral meta-atom, a hierarchical absorber with carbonyl iron particle coating is designed and prepared, of which the total effective absorption bandwidth (EAB, reflection loss ≤−10 dB) amazingly reaches 9.41 GHz, exceeding 199% of the original coatings', and the absorption peak value declines from −15.91 to −32.12 dB. The overall thickness of...