Chinese Journal of Lasers, Volume. 51, Issue 22, 2205001(2024)
Dual‑Wavelength Collimation Metasurface for Rydberg Atomic Sensing Systems
Fig. 1. Comparison of platform and integrated systems. (a) Spatial optical links; (b) typical structure of optical fiber integrated atomic gas chamber; (c) optical fiber end-face integrated metasurface; (d) fiber-to-metasurface bonding
Fig. 3. Transmission phase. (a)‒(b) Phase conditions of dual-wavelength laser collimation metasurface; (c)‒(d) dual-wavelength phase difference
Fig. 4. Metasurface structure. (a) Dual-wavelength laser collimation metasurface; (b) unit cell of metasurface
Fig. 5. Field distribution and amplitude-phase curves. (a) Internal field distribution in dielectric column. (b) variation of transmission phase and amplitude of metasurface unit with width W
Fig. 6. Distribution value of theoretical phase and metasurface unit phase. (a) Theoretical value of 852 nm wavelength beam focusing phase distribution; (b) metasurface unit phase distribution value under irradiation of 852 nm wavelength beam; (c) phase deviation of 852 nm wavelength beam; (d) theoretical value of 510 nm wavelength beam focusing phase distribution; (e) metasurface unit phase distribution value under irradiation of 510 nm wavelength beam; (f) phase deviation of 510 nm wavelength beam
Fig. 7. Transmission phase varies with H. (a) Dual-wavelength transmission phase difference; (b) dual-wavelength transmission phase value; (c)‒(g) phase deviation when H is 1100‒1500 nm
Fig. 8. Transmission phase varies with P. (a) Dual-wavelength transmission phase difference; (b) dual-wavelength transmission phase value; (c)‒(g) phase deviation when P is 230‒270 nm
Fig. 9. Theoretical calculation and simulation results of focusing field distribution. (a) Focused field distribution of beam at wavelengths of 510 nm and 852 nm; (b) field intensity value at center of light field in direction of beam propagation
Fig. 10. Theoretical calculation and simulation results of focusing field. (a) Field intensity value at center of light field in direction of 510 nm wavelength beam propagation; (b) Field intensity value at center of light field in direction of 852 nm wavelength beam propagation
Fig. 11. Dual-wavelength focusing when F=100 μm and metasurface size is 50 μm×50 μm. (a)(b) Focusing field; (c)(d) focal cross section light intensity distribution
Fig. 13. Achromatic performance of light beams of different wavelengths. (a) Confocal collimation of 480 nm and 780 nm wavelength beams; (b) phase deviation of beam in wavelength range of 600~1200 nm (relative to 500 nm)
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Zhanshan Sun, Di Sang, Qiang An, Yi Lin, Yunqi Fu. Dual‑Wavelength Collimation Metasurface for Rydberg Atomic Sensing Systems[J]. Chinese Journal of Lasers, 2024, 51(22): 2205001
Category: Beam transmission and control
Received: Mar. 6, 2024
Accepted: Apr. 19, 2024
Published Online: Nov. 15, 2024
The Author Email: Fu Yunqi (yunqifu@nudt.edu.cn)
CSTR:32183.14.CJL240660