Regarding these applications, high-performance THz devices become essential for manipulating THz light. One crucial group of devices was associated with driving polarization, such as wave retarders, polarizers, and rotators of polarization. [2] Conventional polarization converters used total internal reflection or birefringence effects in polymers and crystals, [3,4] which produced phase retardation. Those wave converters demanded a relatively long propagation distance to achieve the necessary phase accumulation between two orthogonal polarization constituents, leading to bulky size. [3,5] Hence, these approaches were not proper for device integration and miniaturization. Lightweight and compact polarization converters are needed to manipulate the polarization state of the THz wave. In the last decade, metamaterials, i.e., artificial ultrathin subwavelength resonators array, have attracted increasing attention owing to their extraordinary electromagnetic characteristics unavailable in natural materials. [6,7] It opened up meaningful chances, including an alternative approach to control the polarization of light. Recently, the THz metamaterials have made significant progress. [8][9][10] Particularly, polarimetric meta-devices have attracted much attention in the THz region owing to the shortage of proper natural materials for THz device applications. [11,12] To extend the function, broadband metamaterial polarization retarders or converters were highly required. For example, wideband metasurface circular polarizers were shown in the optical region using stacked nanorod arrays [13] and gold helix structures. [14] The metasurfaces have also demonstrated an ability to turn the THz wave's linear polarization state into its orthogonal state in a broadband spectrum. [12,15] For example, Grady et al. presented that between 0.8 and 1.36 THz, the cross-polarized reflection is more significant than 80%, while the co-polarized one is less than 5%. [12] The metamaterial polarization rotation was also proposed to revolve the polarization axis of a linearly polarized THz wave by any angle, and the rotation took place with a conversion efficiency of ≈0.85 at a wideband spectrum. [15] However, further developments of THz polarization meta-converters have been restricted mainly due to the lack of tunability. Their polarization conversion feature cannot be changed once the Polarization is a fundamental characteristic of light waves carrying sensitive measurement and signal communication information. Traditional schemes for advanced controlling polarization impose stringent requirements on material features and obtain merely limited performance. Integration of diversified and switchable functions into monolithic metamaterials has become a rising research field, particularly for the terahertz (THz) spectrum. However, the study on the switchable and wearable polarization meta-converter with nonvolatile operation stays unexplored. Here, the switching of metamaterialinduced ultra-broadband and very efficient reflective linear polarizati...