With the advances in THz technologies, THz functional devices and integrated systems put forward higher requirements for the development of filters, attenuators and absorbers, whose performance is dependent on the absorption characteristics of the device to the incident THz waves. [12] Therefore, absorbers have gained much interests among THz devices, and become one of the most important components for the applications mentioned above. Wide bandwidth coverage and high power absorptance are critical considerations to evaluate the performances of THz absorbers. These capabilities, however, are not readily available via the use of natural bulk materials. To be more specific, the refractive index of traditional bulk materials is typically greater than unity. [13] For materials that are widely used in THz systems, the refractive index of highresistivity silicon is approximately 3.4, [14] and the values for organic materials such as Polydimethylsiloxane (PDMS), [15,16] Polyethylene terephthalate (PET) and Polymide are between 1.5 and1.8. [17] Therefore, these materials are not ideal for THz absorbers as the former faces considerable surface reflections, [18] while the latter generally have low