fabrication facilities or complicated optical design and its transfer efficiency is still challenging to apply to most metasurfaces. [4,19,20] Dielectric metasurfaces have shown many advantages. However, due to the fabrication technology, many geometrical metasurfaces designed for the multiplexing, [5] hologram, [19] beam shaping, [21] and active emission control [22] are based on the metallic design and transmission mode. These designs are fundamentally limited by the diffraction efficiency of the nanoantennas. (summary of the metasurface efficiency can be found in the Supporting Information). The low transfer efficiency leads to a large drawback of the metasurface design: the zero-order intensity is mixed into the output signal, which is due to the unmodulated light. Optical devices require clean and pure output signals. For this reason, optical filters and other components are required to eliminate the noise in almost every experiment. [2,4,5,16,[19][20][21][22] However, one of the ultimate goals for metasurface is to achieve light modulation with an all-in-one ultrathin device, which can replace the bulky and complicated conventional components. These extra noise-reduction measures sacrifice the unique advantages of metasurfaces, reduce the reliability, and greatly limit its functionality in the region close to the metasurface, which becomes a primary weakness compared to classic optical components. In the pursuit to replace the classic optical components with metasurfaces, it becomes a fundamental challenge that requires a novel solution. It is also a barrier for future applications, such as integrated photonics and super-resolution supercritical lens. [10,[23][24][25] In this work, we present design principles for the first self-filtering metasurface with pure modulated light. Via the unprecedented control of the wavefront, it is possible to modify the internal total reflection as a barrier to block the unmodulated light. Unmodulated light contributes most of the noise. In our scheme, these noises are totally reflected at the interface so only the pure modulated light can transmit and propagate. [26] Thus, it is convenient to denote this functional device as Total Reflection Metasurface (TRM). TRM has many advantages to approach the goal of all-in-one metasurfaces. Such self-filtering functional device is insensitive to light polarization. Normal metasurface system requires the polarizer, metasurface, and optical filter to function. TRM integrates these components into an ultrathin design that can be directly plug-to-use. Without the help of extra components, the quality of the component can exceed its classic optical counterparts. Furthermore, based on the concept of TRM, we design an optical cavity strategy to Metasurface has been proposed as one critical platform for orbital angular momentum (OAM) multiplexing. While metasurfaces have unique advantages to achieve light modulation with an ultrathin 2D layer, the relatively low transfer efficiency is a primary drawback. Such weakness leads to the mixing of...