Extensive MRO CRISM observations of 1.27 μ m O 2 airglow in Mars polar night and their comparison to MRO MCS temperature profiles and LMD GCM simulations
Author(s) -
Clancy R. Todd,
Sandor Brad J.,
Wolff Michael J.,
Smith Michael D.,
Lefèvre Franck,
Madeleine JeanBaptiste,
Forget Francois,
Murchie Scott L.,
Seelos Frank P.,
Seelos Kim D.,
Nair Hari A.,
Toigo Anthony D.,
Humm David,
Kass David M.,
Kleinböhl Armin,
Heavens Nicholas
Publication year - 2012
Publication title -
journal of geophysical research: planets
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/2011je004018
Subject(s) - mars exploration program , atmospheric sciences , martian , polar , airglow , atmosphere of mars , latitude , radiative transfer , orbiter , physics , environmental science , astrobiology , astronomy , quantum mechanics
The Martian polar night distribution of 1.27 μ m (0–0) band emission from O 2 singlet delta [O 2 ( 1 Δ g )] is determined from an extensive set of Mars Reconnaissance Orbiter (MRO) Compact Reconnaissance Imaging Spectral Mapping (CRISM) limb scans observed over a wide range of Mars seasons, high latitudes, local times, and longitudes between 2009 and 2011. This polar nightglow reflects meridional transport and winter polar descent of atomic oxygen produced from CO 2 photodissociation. A distinct peak in 1.27 μ m nightglow appears prominently over 70–90NS latitudes at 40–60 km altitudes, as retrieved for over 100 vertical profiles of O 2 ( 1 Δ g ) 1.27 μ m volume emission rates (VER). We also present the first detection of much (×80 ± 20) weaker 1.58 μ m (0–1) band emission from Mars O 2 ( 1 Δ g ). Co‐located polar night CRISM O 2 ( 1 Δ g ) and Mars Climate Sounder (MCS) (McCleese et al., 2008) temperature profiles are compared to the same profiles as simulated by the Laboratoire de Météorologie Dynamique (LMD) general circulation/photochemical model (e.g., Lefèvre et al., 2004). Both standard and interactive aerosol LMD simulations (Madeleine et al., 2011a) underproduce CRISM O 2 ( 1 Δ g ) total emission rates by 40%, due to inadequate transport of atomic oxygen to the winter polar emission regions. Incorporation of interactive cloud radiative forcing on the global circulation leads to distinct but insufficient improvements in modeled polar O 2 ( 1 Δ g ) and temperatures. The observed and modeled anti‐correlations between temperatures and 1.27 μ m band VER reflect the temperature dependence of the rate coefficient for O 2 ( 1 Δ g ) formation, as provided in Roble (1995).
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