polarization manipulation elements have been the two of the most widely investigated device types because of the essential and indispensable functions of these elements. [5][6][7][8][9] In contrast with the traditional bulky optical lenses, a metalens is a micro/ nanostructured metasurface lens in which the amplitude, phase, and polarization state of the transmitted or reflected electromagnetic waves can be manipulated by the micro/nanostructures at the subwavelength scale based on the effects of surface plasmonic polaritons (SPP) or localized surface plasmonics (LSP), [10][11][12][13][14] Mie resonances, [15] and geometric phase (also known as Pancharatnam-Berry phase, P-B phase), [9,[16][17][18][19][20][21][22][23][24] using which focusing, imaging and/or wavefront manipulation in the transmission or reflection can be achieved. Plasmonic lenses consist of an array of metal plasmonic antennas in which a phase discontinuity related to the geometry and dimension of the metallic antennas appears between the incident electromagnetic wave and the transmitted and/or reflected electromagnetic wave due to the SPP/LSP effects. The ability to generate a spherical wavefront or nondiffracting Bessel beam by an array of gold (Au)_ V-shaped nanoantennas with different geometries and dimensions has been experimentally demonstrated at telecom wavelengths. [13] A dual-polarity metalens consisting of an array of plasmonic dipole antennas on a glass substrate with various orientations has also been experimentally demonstrated, in which a convex or concave lens can be realized with an opposite circular polarized illumination, i.e., either left-handed circular polarization (LCP) or right-handed circular polarization (RCP). [14] Using the similar plasmonic dipoles made of subwavelength metallic nanorods with spatially varying orientations, high-resolution 3D holography can also be achieved. [25] Unlike the plasmonic lens, the all-dielectric metalens based on Mie resonances can also achieve focusing with high efficiency, and a metalens with Si elliptical disks with different dimensions embedded in glass substrate was proposed for this purpose. [15] Recently, the P-B phase has attracted much attention and has been employed in focusing/imaging of the optical metasurface. Unlike the propagation phase, the P-B phase is achieved using azimuth-varied nano/micrograting structures. [26,27] Each nano/microunit (metamolecule) of the metalens is similar to a local half-wave plate (HWP) with different azimuthal angle (θ), so that the circular polarization state of the transmission or reflection is orthogonal to that of the A chiral metalens of circular polarization dichroism (CPD) in the mid-infrared region of 3-5 µm is demonstrated both theoretically and experimentally, in which one of the circularly polarized light beams (either left-handed or righthanded) is transmissively focused at a designed focal length, while the other beam is reflected. The metalens consists of subwavelength helical surface arrays covered by a gold thin film that gives r...