of CPL can serve as a molecule-screening tool. In fact, it is widely used in drug screening to discern effective medical target products from ineffective or even toxic enantiomers. [2] The emerging applications in quantum communication and computing, [3,4] circular dichroism spectroscopy, and polarimetric imaging [5] also demand optical chirality detection. However, conventional solutions for optical chirality detection require multiple optical elements including phase retarders, quarter waveplate (QWP), polarizing beam splitters, and rotating optomechanical components. This is due to the lack of intrinsic chiral response in common semiconductors such as silicon and III-V semiconductors from which photodetectors are made, thus, miniaturization of optical chirality detection devices is challenging. One direction of seeking chirality detecting devices is using intrinsically chiral materials including chiral dyes and liquid crystals. The first organic-semiconductor transistor for chirality detection utilized chiral helicene [6] and hybrid perovskite devices were explored by combining the chiral-sensitive absorbing organic material and inorganic compound to enhance the optoelectronic performance. [7,8] The invention of metamaterials or metasurfaces, that is, fabrication of sub-diffraction-limited nanostructures, enabled chiral optical properties beyond those offered by naturally existing materials. Metamaterials with helical nanostructures, for example, spirals that lack mirror symmetry, exhibit chirality-dependent absorption/transmission, and have been shown to achieve direct chirality detection. [9][10][11][12][13][14] Alternatively, metamaterials and metasurfaces also demonstrated the capability of manipulating polarization states, [15] and could function as ultracompact optical elements including linear/circular polarizers, [11] waveplates/ phase-retarders, [16] and polarizing beam splitters. [17] Fabricating these optical elements on top of conventional photodetectors can resolve the optical chirality [18,19] or extract the full Stokes parameters. [20] Topological insulators (TIs) are a new phase of quantum materials with topological surface states (TSS) on the surface. [21,22] Tetradymites are known as one of the best roomtemperature thermoelectric materials for decades [23][24][25][26] and also have been applied in optoelectronics, [27][28][29] and later proven to be 3D TIs. [30][31][32][33] The spin texture of the TSS electrons is locked to their momentum, so that the spin polarization can be induced