Terahertz (THz) technology has attracted more and more attention due to its wide application prospects in imaging, communication, spectroscopy, and other fields. [1] Thanks to the development of metamaterials and metasurfaces, terahertz functional devices such as absorbers, [2,3] polarizers, [4,5] and filters in refs. [6,7] have been greatly developed. Through elaborate design, one can get devices or structures with certain functions. However, once the structure of the metamaterial is determined and made, its function and performance will be fixed.To solve this problem, materials such as stretchable substrate, [8,9] graphene, [10,11] Dirac semimetal, [12,13] and phase-change material in refs. [14][15][16][17] that can be tuned by external pressure, thermal heating, applied current, or optical pumping are added to the design of metamaterials. This makes metamaterials evolve from passive and lack of real-time tuning to enabling active control of the operating frequency, amplitude, phase, or other properties. Although tunable materials are added, these metamaterials are often limited to one kind of functional tuning.Recently, some devices utilizing graphene, [18][19][20][21] vanadium dioxide (VO 2 ) in refs. [22][23][24][25][26][27][28], and Ge 2 Sb 2 Te 5 (GST) in ref. [29] to achieve dual functions have emerged. Among them, some have the function of switching between the quarter-wave plate and half-wave plate. For example, a hybrid graphene-dielectric metasurface that can switch between a half-wave plate and a quarter-wave plate by applying external biasing voltage was proposed. [19] In addition, some devices can transform between a broadband absorber and a narrowband absorber. Song et al. put forward an absorber with tunable bandwidth by utilizing the characteristic that VO 2 can switch between the amorphous state and the crystalline state. [22] Moreover, some studies combine polarization conversion and absorption into a single metasurface simultaneously. Song et al. proposed a bifunctional metasurface based on VO 2 to achieve broadband absorber and broadband polarization converter. [24] The design idea of this metasurface is to design a typical metal-insulator-metal (MIM) structure, and then add another three-layer structure of VO 2 -insulator-VO 2 on this structure. Through the phase transition of VO 2 , the two functions can be switched. Li et al. also adopted this design idea to realize the conversion between a broadband absorber and broadband polarization converter. [30]