Atmospheric Optical Characteristics in the Area of 30–400 km

• Published in: Remote Sensing
• Main Authors: Boris M. Shevtsov, Andrey N. Perezhogin, Ilya N. Seredkin
• Format: Article in Journal/Newspaper
• Language: English
• Published: MDPI AG 2022
• Subjects: optics of the atmosphere; resonant lidar; laser ionozond; lidar reflections in the thermosphere; coefficient and cross-section of light scattering; ionization; Science; Q; Kamchatka
• Online Access: https://doi.org/10.3390/rs14236108; https://doaj.org/article/ede91a47ffc342da84211e1c35db3989

Extremely weak lidar reflections in the thermosphere, which correlate with ionosonde data, were detected in 2008 and 2017 over Kamchatka during seasons of low aerosol filling of the atmosphere at solar activity minima. Here, these reflections are considered in comparison with mesospheric and stratospheric lidar signals that makes it possible to determine favorable conditions for thermospheric lidar observations. In 2014, it was shown that lines of transitions between the excited states of atomic nitrogen ions fall within the 532 nm lidar signal emission band, and in 2017, lidar reflections in the thermosphere were simultaneously obtained at 561 and 532 nm excited transitions of atomic oxygen and nitrogen ions, thereby the resonant nature of thermospheric lidar reflections was established and confirmed. Here, using lidar signals at wavelengths of 561 and 532 nm in the altitude range of 30–400 km, by solving the inverse problem, we restore the light scattering coefficients corresponding to these wavelengths that makes it possible to compare the optical characteristics of the thermosphere, mesosphere, and upper stratosphere and to determine the relationship between resonant, Rayleigh, and aerosol light scattering at different heights of the atmosphere. In conclusion, using the scattering coefficients in the thermosphere, we find the cross-sections of light scattering at the 561 and 532 nm transitions of atomic oxygen and nitrogen ions and explain why the scattering coefficients for O <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mo>+</mo></msup></semantics></math> , 561 nm are less than for N <math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mrow></mrow><mo>+</mo></msup></semantics></math> , 532 nm, while the concentration of O <math xmlns="http://www.w3.org/1998/Math/MathML" ...