Fig. 1. Design of the metalens. (a) Working principle of the metalens and schematic diagram of the structural unit; (b), (c) Top view and side view of the structural unit, respectively, where period P, diameter D and height H of the dielectric cylinder is marked
Fig. 2. Phase response of the structural unit as a function of period P and diameter D of the dielectric cylinder at the operating wavelengths of (a) 3 μm, (b) 4 μm and (c) 5 μm, respectively. Transmittance of energy flow as a function of period P and diameter D of the dielectric cylinder at the operating wavelengths of (d) 3 μm, (e) 4 μm and (f) 5 μm, respectively. Phase coverage
and average transmittance of energy flow
at (g) 3 μm, (h) 4 μm and (i) 5 μm operating wavelengths, respectively, when the diameter D changes within the allowable range under different period P of the structural unit
(a) 3 μm、(b) 4 μm和(c) 5 μm工作波长下结构单元相位随周期P和介质柱直径D的变化;(d) 3 μm、(e) 4 μm和(f) 5 μm工作波长下能流透过率随周期P和介质柱直径D的变化;(g) 3 μm、(h) 4 μm和(i) 5 μm工作波长下,取不同的周期P,当直径D在允许范围内变化时,对应的结构单元相位覆盖范围
和平均能流透过率
Fig. 3. Phase response of the structural unit as a function of height H and diameter D of the dielectric cylinder at the operating wavelengths of (a) 3 μm, (b) 4 μm and (c) 5 μm, respectively. Transmittance of energy flow as a function of height H and diameter D of the dielectric cylinder at the operating wavelengths of (d) 3 μm, (e) 4 μm and (f) 5 μm, respectively. Phase coverage
and average transmittance of energy flow
at (g) 3 μm, (h) 4 μm and (i) 5 μm operating wavelengths, respectively, when the diameter D changes within the allowable range under different height H of the structural unit
(a) 3 μm、(b) 4 μm和(c) 5 μm工作波长下结构单元产生的相位随介质柱高度H和直径D的变化;(d) 3 μm、(e) 4 μm和(f) 5 μm工作波长下能流透过率随介质柱高度H和直径D的变化;(g) 3 μm、(h) 4 μm和(i) 5 μm工作波长下,取不同的介质柱高度H,当直径D在允许范围内变化时,对应的结构单元相位覆盖范围
和平均能流透过率
Fig. 4. Transmittance of energy flow and phase response of the optimal structural unit at the operating wavelengths of (a) 3 μm, (b) 4 μm and (c) 5 μm (The size of the optimal structural unit at corresponding design wavelengths are marked in the insets)
Fig. 5. The focusing performance of the metalens in the x-z plane at operating wavelengths of 3 μm, 4 μm and 5 μm. (a) λd = 3 μm,f = 98.4 μm, the focusing efficiency is 70.7%; (b) λd = 4 μm,f = 97.7 μm, the focusing efficiency is 70.5%; (c) λd = 5 μm, f = 97 μm, the focusing efficiency is 70.4%; (d)-(f) Normalized energy flow distribution along the x direction at the focal plane (white dotted line in the figure) at the operating wavelengths of 3 μm, 4 μm and 5 μm, and the full width at half-maximum (FWHM) of the focus is marked
Fig. 6. Dispersion characteristics of the metalens within ±0.5 μm of the design wavelength. The metalens with a design wavelength of 3 μm within the 2.5-3.5 μm wavelength range: (a) Normalized energy flow of the light field along the z-axis direction (x = 0), (b) the relationship between the focal position and the incident wavelength. The metalens with a design wavelength of 4 μm within the wavelength range of 3.5-4.5 μm: (c) Normalized energy flow of the light field along the z-axis direction (x = 0), (d) the relationship between the focal position and the incident wavelength. The metalens with a design wavelength of 5 μm within the 4.5-5.5 μm wavelength range: (e) Normalized energy flow of the light field along the z-axis direction (x = 0), (f) the relationship between the focal position and the incident wavelength