Author Affiliations
1School of Electronic Engineering, State Key Laboratory for Information Photonics and Optical Communications, Beijing Key Laboratory of Work Safety Intelligent Monitoring, Beijing University of Posts and Telecommunications, Beijing 100876, China2School of Information, Beijing University of Technology, Beijing 100124, China3Institute of Laser Engineering, Beijing University of Technology, Beijing 100124, Chinashow less
Fig. 1. (Color online) The graded refractive-index structure of an N-layer anti-reflective coating system. A plane wave is incident from the air with the refractive index of n0 and incident angle of θ. Every layer of the coating is characterized by the thickness di with the refractive index ni, i = {1, 2, …, N}. The entire absorption layer is assumed to be in the bottom layer with refractive index nab without the back surface reflectance. The right curve shows the numerical value of the graded change of refractive index and the thickness of each anti-reflective layer.
Fig. 2. (Color online) The dependence of the incident photon flux density on the wavelength and the incident angle on the day of the spring equinox for (a) Quito, (b) Beijing and (c) Moscow, respectively. At noon of the day of the spring equinox, the sunlight is vertically incident on the equator. The incident angle at noon of the day of spring equinox for Quito, Beijing and Moscow is 0, 40, and 55 degrees, respectively. At sunrise or sunset, the incident angles of these three cities are the same 90 degrees. (d) The comparison of the spectrum of the incident photon flux density of three cities at noon on the day of the spring equinox. The incident photon flux density spectra are totally different Earth due to the atmosphere scatter and absorption at different location with different incident angle and latitude.
Fig. 3. (Color online) The optical transmittance spectrum with λ = [300, 1100] nm and θ = [0°, 90°] for two-layer AR coating optimized by (a) ACA without SPCTRL2, and with SPCTRL2 of (b) Quito (c) Beijing and (d) Moscow. The detail structures are presented in Table 2. The areas with transmittance above 80% and 98% are marked by white lines. The incident quantum efficiency at Quito, Beijing and Moscow optimized by ACA with SPCTRL2 incorporated is 0.26%, 1.37% and 4.24% larger than that optimized without SPCTRL2 incorporated for two-layer AR coating, respectively. Comparison of the actual solar spectrum and incident quantum efficiency ηin (λ), for (e) Quito (f) Beijing and (g) Moscow with and without SPCTRL2 incorporated. When considering the solar spectrum in different cities and setting ηin as the evaluation function in the AR coating optimization, the peak of the quantum efficiency spectrum moves towards around 700 nm, which is the peak of the actual solar spectrum and fits the actual solar spectrum very well for all three cities.
Parameter | Latitude
(°)
| Longitude
(°)
| Aerosol
optical depth
| Alpha | Albedo (surface
reflectance)
| Total column
ozone (cm)
| Total precipitable
water vapor (cm)
| Surface
pressure (mB)
| Days of
the year
|
---|
Quito | 0 | 78.5W | 0.27 | 1.14 | 0.2 | 0.34 | 1.42 | 1013.25 | 79 | Beijing | 39.9N | 116.3E | 0.77 | 1.14 | 0.16 | 0.34 | 0.95 | 1040 | 79 | Moscow | 55.3N | 37.5E | 0.35 | 1.14 | 0.1 | 0.36 | 1.36 | 750 | 79 |
|
Table 1. Input parameters used in SPCTRL2 program.
Optimization method | 1st layer | | 2nd layer |
---|
Refractive index | Thickness (nm) | | Refractive index | Thickness (nm) |
---|
No SPCTRL2 | 1.41 | 112.09 | | 2.41 | 58.89 | SPCTRL2 at Quito | 1.44 | 113.66 | 2.55 | 60.46 | SPCTRL2 at Beijing | 1.27 | 165.29 | 2.29 | 76.10 | SPCTRL2 at Moscow | 1.17 | 221.62 | | 2.15 | 80.80 |
|
Table 2. Detail structures of two-layer antireflective coating optimized by ant colony algorithm with and without SPCTRL2 incorporated.