has made realistic applications of the THz wave very limited. Among the functional THz devices, perfect absorbers are highly desirable in manipulating the THz wave in a number of important fields.In recent years, extensive efforts have been devoted to perfect THz absorption based on artificial structures, such as metasurfaces. [2][3][4] Most of these structures, however, were passive devices and incapable of real-time adjustment. Graphene, a 2D sheet of hexagonally arranged carbon atoms, has attracted much attention in the past decade due to its extraordinary electronic and optoelectronic properties. [5] As a 2D semiconductor, its electron mobility and Fermi level can be extensively controlled by external stimulants, such as gate voltage [6] and thus its surface conductivity. Therefore, graphene has been a promising candidate for active optoelectronics applications and absorber devices based on demonstrations in the microwave [7,8] and infrared [9][10][11][12][13][14][15][16][17][18] regimes. At THz frequencies, graphene-based absorbers were also experimentally realized. By integrating monolayer graphene into a classical Salisbury screen structure, perfect THz absorption was achieved. [19][20][21][22] However, the graphene Fermi level needed to realize perfect absorption was very high and the thickness of the absorbers were required to be around λ/4, which is too bulky for optical integration. A broadband, nearly perfect THz absorber based on patterned graphene was also reported [23] with a relatively small electrical tunability. Besides, theoretical works on graphene-based THz absorbers were proposed. [24][25][26][27][28][29] However, most studies mainly focused on simulations and calculations. Therefore, experimental realization of electrically tunable perfect THz absorption based on lightly-doped and low-quality graphene with deep subwavelength dimensions remains as an unsolved challenge.In this article, we experimentally demonstrate an electrically tunable perfect THz absorber by integrating a metallic grating into a graphene-based Salisbury screen structure. The measured results show that perfect absorption can be achieved with a more lightly doped chemical vapor deposition (CVD) graphene compared to that of the classical Salisbury screen absorber and the modulation depth of absorbance can reach up to 25%. Numerical simulations were performed using commercial full-wave numerical software showing a good agreement with the measurements. Furthermore, we proposed a simple Graphene, as a popular 2D semiconductor, with a carrier concentration that can be extensively tailored by external stimulants, such as electric bias and photoexcitation, is a promising candidate for active optoelectronics. An electrically tunable perfect terahertz absorber is presented by integrating a metallic grating into classical graphene Salisbury screen. The measurement shows that perfect absorption can be achieved for even lightly-doped graphene and a modulation depth up to 25% is realized. Numerical simulation and analytical model based...