Abstract:International audienceUltraviolet (UV) spectra of the δ (190-240 nm) and γ (225-270 nm) bands of the nitric oxide (NO) molecule have been measured on the nightside of the atmosphere of Venus with the Spectroscopy for Investigation of Characteristics of the Atmosphere of Venus (SPICAV) instrument on board Venus Express (VEX). Excited NO molecules on the nightside of the planet are created by radiative recombination of O(3P) and N(4S) atoms. The atoms are produced by photodissociation of CO2 and N2 molecules on … Show more
“…These were detected by the International Ultraviolet Explorer (IUE) and the Pioneer Venus UV instrument as well as by the SPICAV instrument onboard Venus Express (Stiepen et al, 2012(Stiepen et al, , 2013. Another reaction is combination of excited state N atoms with CO 2 to form NO (below).…”
“…These were detected by the International Ultraviolet Explorer (IUE) and the Pioneer Venus UV instrument as well as by the SPICAV instrument onboard Venus Express (Stiepen et al, 2012(Stiepen et al, , 2013. Another reaction is combination of excited state N atoms with CO 2 to form NO (below).…”
“…In 2012, Stiepen et al . [] published results from a statistical study of the NO airglow based on a larger data set for the Northern Hemisphere from Gérard et al . [].…”
Section: Discussionmentioning
confidence: 99%
“…Analyses derived from the Venus Express data [ Gérard et al ., ; Royer et al ., ; Stiepen et al ., ] have shown that the NO emission peaks at a mean altitude of 113 km, with the NO airglow being observed in the 95 to 132 km range. The limb brightness was found to range between 5 kR and 540 kR and the scale height to be about 8 km.…”
Section: Introductionmentioning
confidence: 99%
“…Both data sets are thus complementary. In 2012,Stiepen et al [2012] published results from a statistical study of the NO airglow based on a larger data set for the Northern Hemisphere fromGérard et al [2008]. A second study fromStiepen et al [2013] focused on nadir observations made by SPICAV.…”
We present results from a NO airglow inversion method based on Venus Express data acquired from 2006 to 2010, during the last solar minimum period. We retrieve an altitude of 114 ± 10 km for the emission peak of the NO layer, with an associated scale height of 20 ± 10 km and an average limb brightness of 59.3 kR with a standard deviation of 63 kR. The inversion method allows for the quantification of the horizontal homogeneity of the NO layer. Images of the SPICAV field of view show a great variability of airglow morphologies, with NO layers that can be horizontally homogenous and continuous over distances exceeding 100 km, as well as sporadic patches of NO on a smaller horizontal scale. Frequent secondary emissions seen at lower tangent altitudes are the signatures of the complex dynamics of the upper Venusian atmosphere.
“…In all these cases, the measured horizontal wavelengths and phase velocities have been demonstrated to be comparable with GWs propagating at the considered altitudes [ Peralta et al ., , ]. Occasional secondary peaks, probably induced by GW propagations, were also observed above the main peak of the NO nightglow from SPICAV (Spectroscopy for Investigation of Characteristics of the Atmosphere of Venus) data [ Stiepen et al ., ]. The effect of planetary waves in the O 2 nightglow intensity fluctuation was investigated by Hoshino et al .…”
In this work we describe a model of the perturbation of the O 2 (a 1 Δ g ) nightglow limb profiles by the action of gravity waves (GWs) propagating in the Venus' upper atmosphere. Data have been acquired by the Visible and InfraRed Thermal Imaging Spectrometer (VIRTIS) on board the European Space Agency mission Venus Express (VEX). The high variability observed in the shape of the O 2 (a 1 Δ g ) nightglow limb profiles between 80 and 120 km, often characterized by the presence of a double peak, suggests the occurrence of GWs at the considered altitudes. In order to model and derive the GWs properties, we apply to Venus a well-known theory used to study terrestrial density fluctuations induced by the GWs propagation. The retrieved vertical wavelengths and amplitudes of the waves at the O 2 (a 1 Δ g ) layer altitude (~100 km) are of the order of 7-16 km and 3-14% respectively, complying with wave amplitude threshold for dynamical instability in the majority of the fitted cases. Temperature fluctuations would exceed 40% at higher altitudes (115-120 km) thus inducing either wave breaking or dissipation. Intrinsic horizontal phase velocities are expected to vary in the range 32 m/s and 85 m/s. GWs are detected in a wide range of latitudes from the midlatitudes up to the polar regions, and we cannot exclude existence of the sources of different nature. This study also confirms the high variability induced by the action of GW propagation in the airglow profiles of the terrestrial planets and points out the need for future missions to couple simultaneous complementary GW detection techniques in order to better constrain GW properties and understand their impact on the Venus general circulation.
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