atmospheric windows
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2021 ◽  
Author(s):  
Ting Xie ◽  
Fei Zhang ◽  
Hanlin Bao ◽  
Mingbo Pu ◽  
Yinghui Guo ◽  
...  

2021 ◽  
pp. 105055
Author(s):  
Wen-zhuang Ma ◽  
Jing Liu ◽  
Wei Chen ◽  
Yu-shan Chen ◽  
Ping-Ping Zhuang ◽  
...  

Atmosphere ◽  
2021 ◽  
Vol 12 (9) ◽  
pp. 1119
Author(s):  
Roger Vilà ◽  
Marc Medrano ◽  
Albert Castell

Radiative cooling is a natural process to cool down surfaces through the rejection of thermal radiation using the outer space as a cold sink, taking advantage of the transparency of the atmospheric windows (8–14 μm), which partially matches the infrared radiation band. With the development of new materials that have a high reflectivity of solar radiation, daytime radiative cooling can be achieved. This phenomenon depends on the optical properties of the surface and the local weather conditions. In this research, climatological data from 1791 weather stations were used to present detailed nighttime and all-day radiative cooling maps for the potential implementation of radiative cooling-based technologies. The paper offers a parametric study of the variation of the potential as a result of decreasing the solar reflectivity. The results show that southern Europe is the region with the highest potential while northern Europe holds more hours of available radiative cooling. After varying the solar reflectivity from 1 to 0.5 the average power reduces from 60.18 to 45.32 W/m2, and energy from 527.10 to 264.87 kWh/m2·year. For solar reflectivity lower than 0.5, all-day radiative coolers behave as nighttime radiative coolers, but power and energy values improve significantly for high values of solar reflectivity. Small variations of solar reflectivity have greater impacts on the potential at higher reflectivity values than at lower ones.


2021 ◽  
Author(s):  
Alan Symmons ◽  
Mark Lifshotz
Keyword(s):  

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Claire Fourmentin ◽  
Xiang-Hua Zhang ◽  
Enora Lavanant ◽  
Thierry Pain ◽  
Mathieu Rozé ◽  
...  

AbstractIn order to decrease the number of lenses and the weight of thermal imaging devices, specific optical design are required by using gradient refractive index (GRIN) elements transparent in the infrared waveband. While widely used for making visible GRIN lenses with silicate glasses, the ion exchange process is very limited when applied to chalcogenide glasses due to their low Tg and relatively weak mechanical properties. In this paper, we develop chalco-halide glasses based on alkali halide (NaI) addition in a highly covalent GeSe2–Ga2Se3 matrix, efficient for tailoring a significant and permanent change of refractive by ion exchange process between K+ and Na+. Optical and structural properties of the glass samples were measured showing a diffusion length reaching more than 2 mm and a Gaussian gradient of refractive index Δn of 4.5.10–2. The obtained GRIN lenses maintain an excellent transmission in the second (3–5 µm) and third (8–12 µm) atmospheric windows.


2020 ◽  
Vol 641 ◽  
pp. A44
Author(s):  
L. Morelli ◽  
V. D. Ivanov ◽  
A. Pizzella ◽  
D. Gasparri ◽  
L. Coccato ◽  
...  

Context. Stellar population studies in the infrared (IR) wavelength range have two main advantages with respect to the optical regime: they probe different populations, because most of the light in the IR comes from redder and generally older stars, and they allow us to see through dust because IR light is less affected by extinction. Unfortunately, IR modeling work was halted by the lack of adequate stellar libraries, but this has changed in the recent years. Aims. Our project investigates the sensitivity of various spectral features in the 1−5 μm wavelength range to the physical properties of stars (Teff, [Fe/H], log g) and aims to objectively define spectral indices that can characterize the age and metallicity of unresolved stellar populations. Methods. We implemented a method that uses derivatives of the indices as functions of Teff, [Fe/H] or log g across the entire available wavelength range to reveal the most sensitive indices to these parameters and the ranges in which these indices work. Results. Here, we complement the previous work in the I and K bands, reporting a new system of 14, 12, 22, and 12 indices for Y, J, H, and L atmospheric windows, respectively, and describe their behavior. We list the equivalent widths of these indices for the Infrared Telescope Facility (IRTF) spectral library stars. Conclusions. Our analysis indicates that features sensitive to the effective temperature are present and measurable in all the investigated atmospheric windows at the spectral resolution and in the metallicity range of the IRTF library for a signal-to-noise ratio greater than 20−30. The surface gravity is more challenging and only indices in the H and J windows are best suited for this. The metallicity range of the stars with available spectra is too narrow to search for suitable diagnostics. For the spectra of unresolved galaxies, the defined indices are valuable tools in tracing the properties of the stars in the IR-dominant stellar populations.


2020 ◽  
Vol 1 (1) ◽  
pp. 24 ◽  
Author(s):  
Jason W. Barnes ◽  
Shannon M. MacKenzie ◽  
Eliot F. Young ◽  
Jason M. Soderblom ◽  
Alexander G. Hayes ◽  
...  

2020 ◽  
Vol 45 (10) ◽  
pp. 2800 ◽  
Author(s):  
Jihua Zhang ◽  
Ran Wei ◽  
Mohamed ElKabbash ◽  
E. Michael Campbell ◽  
Chunlei Guo

Author(s):  
Magdalene Wan Ching Goh

Electromagnetic wave propagation is an invisible phenomenon that cannot be detected by the human senses. To understand wave propagation, one must first learn what wave propagation is and the basic principles that affect wave propagation. This chapter introduces the atmospheric windows which allow electromagnetic radiation from bands to penetrate Earth. Helmholtz equations, i.e. the equations which govern wave propagation, and the properties of waves (such as propagation constant and characteristic impedance) are then briefly explained. When waves encounter different media during its propagation, they may be reflected, refracted, or diffracted. These phenomena are also covered. The last part of this chapter concisely explains the terminologies commonly used to describe electromagnetic radiation.


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