Standard

Photolysis of O3 at Hartley, Chappuis, Huggins, and Wulf Bands in the Middle Atmosphere: Vibrational Kinetics of Oxygen Molecules O2(X3Σg, ν ≤ 35). / Yankovsky, V. A.; Babaev, A.S.

в: Atmospheric and Oceanic Optics, Том 24, № 1, 2011, стр. 6-16.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

APA

Vancouver

Author

BibTeX

@article{86fbbd42c108491a83acc154ef521f9f,
title = "Photolysis of O3 at Hartley, Chappuis, Huggins, and Wulf Bands in the Middle Atmosphere: Vibrational Kinetics of Oxygen Molecules O2(X3Σg, ν ≤ 35)",
abstract = "Abstract—The advanced version of the full model of O2 and O3 photodissociation in the mesosphere and thermosphere (Yankovsky V.A., Manuilova R.O., Atmospheric and Oceanic optics, 2003, V. 16, No. 7, P. 582) was used for the calculation of vertical profiles of vibrationally excited O2(X, ν) molecular concentrations in the ground electronic state for ν = 1–35. Recent data on the rate constants for reactions O2(X, ν ≤ 30) + O(3P) → O2(X, ν' <ν) + O(3P) and O2(X, ν) were included for the first time in this model. These reactions play a significant role not only in the quenching of O2(X, ν) molecules, but also in the population of under lying vibrational levels of O2 molecules. In addition to direct processes of the production of O2(X, ν ≤ 35), resulting from O3 photolysis, the processes of population of O2(X, ν ≤ 9) molecules through the energy transfer from O(1D), O2(b, ν ≤ 2), and O2(a, ν ≤ 5) were used in the model. The resulting quantum output (RQO) for O2(X, ν = 1) molecules in process of ozone photolysis i",
keywords = "ozone, photolysis, Hartley, Chappuis, Huggins, and Wulf Bands, vibrational kinetics of oxygen molecules, mesosphere, low thermosphere",
author = "Yankovsky, {V. A.} and A.S. Babaev",
year = "2011",
doi = "10.1134/S1024856011010155",
language = "English",
volume = "24",
pages = "6--16",
journal = "Atmospheric and Oceanic Optics",
issn = "1024-8560",
publisher = "Springer Nature",
number = "1",

}

RIS

TY - JOUR

T1 - Photolysis of O3 at Hartley, Chappuis, Huggins, and Wulf Bands in the Middle Atmosphere: Vibrational Kinetics of Oxygen Molecules O2(X3Σg, ν ≤ 35)

AU - Yankovsky, V. A.

AU - Babaev, A.S.

PY - 2011

Y1 - 2011

N2 - Abstract—The advanced version of the full model of O2 and O3 photodissociation in the mesosphere and thermosphere (Yankovsky V.A., Manuilova R.O., Atmospheric and Oceanic optics, 2003, V. 16, No. 7, P. 582) was used for the calculation of vertical profiles of vibrationally excited O2(X, ν) molecular concentrations in the ground electronic state for ν = 1–35. Recent data on the rate constants for reactions O2(X, ν ≤ 30) + O(3P) → O2(X, ν' <ν) + O(3P) and O2(X, ν) were included for the first time in this model. These reactions play a significant role not only in the quenching of O2(X, ν) molecules, but also in the population of under lying vibrational levels of O2 molecules. In addition to direct processes of the production of O2(X, ν ≤ 35), resulting from O3 photolysis, the processes of population of O2(X, ν ≤ 9) molecules through the energy transfer from O(1D), O2(b, ν ≤ 2), and O2(a, ν ≤ 5) were used in the model. The resulting quantum output (RQO) for O2(X, ν = 1) molecules in process of ozone photolysis i

AB - Abstract—The advanced version of the full model of O2 and O3 photodissociation in the mesosphere and thermosphere (Yankovsky V.A., Manuilova R.O., Atmospheric and Oceanic optics, 2003, V. 16, No. 7, P. 582) was used for the calculation of vertical profiles of vibrationally excited O2(X, ν) molecular concentrations in the ground electronic state for ν = 1–35. Recent data on the rate constants for reactions O2(X, ν ≤ 30) + O(3P) → O2(X, ν' <ν) + O(3P) and O2(X, ν) were included for the first time in this model. These reactions play a significant role not only in the quenching of O2(X, ν) molecules, but also in the population of under lying vibrational levels of O2 molecules. In addition to direct processes of the production of O2(X, ν ≤ 35), resulting from O3 photolysis, the processes of population of O2(X, ν ≤ 9) molecules through the energy transfer from O(1D), O2(b, ν ≤ 2), and O2(a, ν ≤ 5) were used in the model. The resulting quantum output (RQO) for O2(X, ν = 1) molecules in process of ozone photolysis i

KW - ozone

KW - photolysis

KW - Hartley

KW - Chappuis

KW - Huggins

KW - and Wulf Bands

KW - vibrational kinetics of oxygen molecules

KW - mesosphere

KW - low thermosphere

U2 - 10.1134/S1024856011010155

DO - 10.1134/S1024856011010155

M3 - Article

VL - 24

SP - 6

EP - 16

JO - Atmospheric and Oceanic Optics

JF - Atmospheric and Oceanic Optics

SN - 1024-8560

IS - 1

ER -

ID: 5062750