wavelength of incoming light to accumulate 0 to π phase shifts. That means subwavelength compact planar geometry is not possible in conventional lenses making optical systems bulky. Furthermore, conventional lenses are limited by optical aberrations (e.g., spherical and chromatic) and diffraction limit. [1] The Abbe-Rayleigh diffraction limit is a natural obstacle in conventional optical lenses due to the far-field interference and absence of near-field. [2] Various planar lenses have been demonstrated following the diffractive optics concept of phase control based on dielectric scatterers on a 2D plane. [3][4][5][6][7][8][9] However, in the mid-infrared wavelength range (3-16 µm), such engineered dielectric surfaces are elusive due to the low spectral bandwidth [8,9] and high thermal noise in long wavelengths. [10,11] In contrast, plasmonic nanoantennas [12][13][14][15][16][17] enable abrupt change in phase, amplitude, and polarization of the incident light using subwavelength optical scatterers on a planar surface. Such control of phase according to the Huygens principle [18] allows the formation of arbitrary wavefront shapes enabling subwavelength focusing. [3][4][5] Spatially distributed plasmonic nanoantennas suppress higher diffraction orders and concentrate the incident light beam beyond the Abbe-Rayleigh diffraction limited focal point. [19][20][21][22] In addition, possibility of the optical impedance matching with the free space by the patterned plasmonic interface reduces back scattering, leading to higher transmission efficiency. [5,23] Going beyond the Abbe-Rayleigh diffraction limit requires the involvement of evanescent fields with large spatial frequency components which is possible by plasmonic nanoantennas, enabling subwavelength resolution capability going beyond the current imaging technologies. [2,14,22,24,25] Here, we propose and experimentally demonstrate an ultrathin flat lens working in the mid-IR spectral range with geometrically tunable focal length and subwavelength focusing ability. The transmission efficiency of this flat lens is substantially higher compared with other reported plasmonic lenses due to the low metallic fill-fraction and the geometry. [14][15][16]26,27] The biggest limitation of dielectric as well as metallic flat lenses is the bandwidth of operation due to the inherent narrowband resonance. [8,9] Previously, reported plasmonic flat lenses were limited to λ ≈ 1.0-1.9 µm, [15] ≈5.2-9.9 µm, [16] and λ ≈ 5-10 µm, [14] operation bandwidths in the infrared spectral range. None of these works reported the most critical lens Integrated photonic circuits and infrared imaging systems demand compact optical components. Dielectric diffractive optics enables miniaturization of the curved refractive optics into planar structure by encoding phase over a 2D plane. However, in the mid-infrared wavelength range, such engineered dielectric surfaces are not efficient, because optically transparent dielectric scatterers with high index contrast in the mid-infrared spectral range suffer f...