the concept of superoscillation, [13,14] there has been growing interest in developing optical super-resolution devices for far-field operation without evanescent waves. [15,16] According to this concept, an arbitrary small point-spread function (PSF) can be achieved by engineering the wave front of the incident wave through a properly designed amplitude-phase mask. [17] This opens an alternative way toward far-field optical super-resolution. In the past several years, various types of superoscillatory lenses have been demonstrated, including linear-focusing lenses, [18,19] spot-focusing lenses, [20,21] long-depth-of-focusing lenses, [22][23][24] and vector wave superoscillatory lenses. [25][26][27][28][29][30] So far, the smallest PSF that has ever been experimentally demonstrated has a full-width-at-half-maximum (FWHM) value of 0.33λ, [31] where λ is the working wavelength. Due to their comparative large sidelobes, those super-resolution lenses are not suitable for direct imaging. In most traditional optical imaging systems, super-resolution PSF usually leads to relatively large sidelobes, which carry a decent amount of energy and might restrict further improvement in the spatial resolution. However, in a confocal microscope, the sidelobes of a super-resolution illumination lens can be effectively suppressed by a conventional optical objective lens, because the PSF of the entire confocal optical system is the product of the two PSFs of the illumination lens and the collection lens. [32] Although their focusing efficiency is only several percentages, super-resolution lenses have demonstrated promising potentials in the application Recently, developments in superoscillatory optical devices have allowed for label-free far-field optical super-resolution technology by allowing engineering of optical point-spread functions beyond the traditional Abbe diffraction limit. However, such superoscillatory optical devices are optimized for the normalincident operation, which inevitably leads to a comparatively slow imaging acquisition rate in the application of super-resolution microscopy. Here, a super-resolution metalens is demonstrated with a high numerical aperture that can focus oblique incident light into a hot spot with a size smaller than the diffraction limit at the visible wavelength. This super-resolution metalens has a numerical aperture of as large as 0.97, a focal length of 38.0 µm, a radius of 151.9 µm, and a field of view of 4° that enables super-resolution focusing on the focal plane at a wavelength of λ = 632.8 nm. In a 5.6λ × 5.6λ field of view on the focal plane, the size of the focal spot is smaller than 0.45λ, which is only 0.874 times the corresponding Abbe diffraction limit. The super-resolution metalens offers a promising way toward fast-scanning labelfree far-field super-resolution microscopy.