Abstract:[1] Limb observations with the SPICAM ultraviolet spectrometer on board the Mars Express orbiter revealed ultraviolet nightglow emission in the d (190-240 nm) and g (225-270 nm) bands of nitric oxide. This emission arises from radiative recombination between O( 3 P) and N( 4 S) atoms that are produced on the day side and form excited NO molecules on the night side. In this study, we analyze the night limb observations obtained during the MEX mission. In particular, we describe the variability of the emission b… Show more
“…For each of the 128 occultations that returned a positive NO detection, we proceeded with the inversion technique described in . The resulting data set extends the latitudinal and seasonal coverage beyond that of the data used in the Cox et al [2008] study. As an example, the result of this inversion for orbit #0588A01 is shown in Figure 1.…”
Section: Observationsmentioning
confidence: 99%
“…The technique is described in . The results are then compared with the analysis of the SPICAM limb observations of the NO emission by Cox et al [2008], which is the only published data set for this Mars atmospheric emission and which covered only a limited L s sampling. The observations of the emission are further compared with model simulations of NO airglow to verify our understanding of the photochemical mechanism producing this feature in the Mars atmosphere.…”
Section: Introductionmentioning
confidence: 99%
“…Cox et al [2008] concluded from their analysis that the higher the latitude of the measurements, the lower is the altitude of the peak, which they linked to the behavior of constant pressure surfaces that are higher close to the equator. Also, they found that the highest brightness values are near 60 ı S, but they could not infer a real systematic dependence between the peak altitude and the peak brightness.…”
Section: Introductionmentioning
confidence: 99%
“…We extracted NO signal from 128 of the 2215 occultations, allowing a much better global view than that from the rather sparse dedicated nightglow limb data (29 independent positive detections over 2 years 2004[Cox et al, 2008). The present data set extends from L s = 44 ı for Martian year (MY) 27 to L s =326 ı in MY 29, spanning almost three Martian years in total.…”
Section: Introductionmentioning
confidence: 99%
“…[4] After the 2005 NO discovery, Cox et al [2008] analyzed 21 orbits of SPICAM containing limb observations of these NO UV emissions: The maximum brightness of the observations is in the range 0.2 to 10.5 kR, with a mean value of 1.2˙1.5 kR, and it peaks between 55 and 92 km in altitude, with a mean value of 73.0˙8.2 km. Cox et al [2008] concluded from their analysis that the higher the latitude of the measurements, the lower is the altitude of the peak, which they linked to the behavior of constant pressure surfaces that are higher close to the equator.…”
[1] We report observations of NO nightglow with the Spectroscopy for the Investigation of the Characteristics of the Atmosphere of Mars (SPICAM) experiment on board the Mars Express (MEx) spacecraft. NO molecules emit an ultraviolet photon when N and O atoms (produced at high altitude in the thermosphere) recombine. Therefore, this emission is a tracer of the atmospheric dynamics in the lower thermosphere where O and N atoms are produced, and below, in the altitude region 50-100 km where the emission is detected. A new retrieval method has been developed to analyze the measurements from this instrument in the stellar occultation mode without slit and retrieve the absolute brightness of the emission. We present the results from the processing of more than 2000 orbits, providing the first global latitude-season distribution of the emission, established over three Martian years. The results are globally consistent with previously available measurements of dedicated limb nightglow obtained during the first Martian year of MEx (MY27). We compared the ensemble of both data sets with the predictions of the Laboratoire de Météorologie Dynamique Mars General Circulation Model (LMD-MGCM), with the addition of the full chemistry of N atoms. We find an overall agreement between the observed and modeled airglow intensities, but discrepancies are also found. The frequency and magnitude of the NO airglow observations show important asymmetries between the Northern and the Southern Hemispheres. There is no detection of emission near the poles during equinox conditions, while the model predicts that it should be most intense because of a circulation with two descending branches at the poles.
“…For each of the 128 occultations that returned a positive NO detection, we proceeded with the inversion technique described in . The resulting data set extends the latitudinal and seasonal coverage beyond that of the data used in the Cox et al [2008] study. As an example, the result of this inversion for orbit #0588A01 is shown in Figure 1.…”
Section: Observationsmentioning
confidence: 99%
“…The technique is described in . The results are then compared with the analysis of the SPICAM limb observations of the NO emission by Cox et al [2008], which is the only published data set for this Mars atmospheric emission and which covered only a limited L s sampling. The observations of the emission are further compared with model simulations of NO airglow to verify our understanding of the photochemical mechanism producing this feature in the Mars atmosphere.…”
Section: Introductionmentioning
confidence: 99%
“…Cox et al [2008] concluded from their analysis that the higher the latitude of the measurements, the lower is the altitude of the peak, which they linked to the behavior of constant pressure surfaces that are higher close to the equator. Also, they found that the highest brightness values are near 60 ı S, but they could not infer a real systematic dependence between the peak altitude and the peak brightness.…”
Section: Introductionmentioning
confidence: 99%
“…We extracted NO signal from 128 of the 2215 occultations, allowing a much better global view than that from the rather sparse dedicated nightglow limb data (29 independent positive detections over 2 years 2004[Cox et al, 2008). The present data set extends from L s = 44 ı for Martian year (MY) 27 to L s =326 ı in MY 29, spanning almost three Martian years in total.…”
Section: Introductionmentioning
confidence: 99%
“…[4] After the 2005 NO discovery, Cox et al [2008] analyzed 21 orbits of SPICAM containing limb observations of these NO UV emissions: The maximum brightness of the observations is in the range 0.2 to 10.5 kR, with a mean value of 1.2˙1.5 kR, and it peaks between 55 and 92 km in altitude, with a mean value of 73.0˙8.2 km. Cox et al [2008] concluded from their analysis that the higher the latitude of the measurements, the lower is the altitude of the peak, which they linked to the behavior of constant pressure surfaces that are higher close to the equator.…”
[1] We report observations of NO nightglow with the Spectroscopy for the Investigation of the Characteristics of the Atmosphere of Mars (SPICAM) experiment on board the Mars Express (MEx) spacecraft. NO molecules emit an ultraviolet photon when N and O atoms (produced at high altitude in the thermosphere) recombine. Therefore, this emission is a tracer of the atmospheric dynamics in the lower thermosphere where O and N atoms are produced, and below, in the altitude region 50-100 km where the emission is detected. A new retrieval method has been developed to analyze the measurements from this instrument in the stellar occultation mode without slit and retrieve the absolute brightness of the emission. We present the results from the processing of more than 2000 orbits, providing the first global latitude-season distribution of the emission, established over three Martian years. The results are globally consistent with previously available measurements of dedicated limb nightglow obtained during the first Martian year of MEx (MY27). We compared the ensemble of both data sets with the predictions of the Laboratoire de Météorologie Dynamique Mars General Circulation Model (LMD-MGCM), with the addition of the full chemistry of N atoms. We find an overall agreement between the observed and modeled airglow intensities, but discrepancies are also found. The frequency and magnitude of the NO airglow observations show important asymmetries between the Northern and the Southern Hemispheres. There is no detection of emission near the poles during equinox conditions, while the model predicts that it should be most intense because of a circulation with two descending branches at the poles.
We present 10 years of Martian NO nightglow Spectroscopy for Investigation of Characteristics of the Atmosphere of Mars observations in limb and stellar occultation modes. The NO nightglow is used as a tracer of the summer-to-winter hemispherical circulation in the upper atmosphere of Mars. Its distribution roughly follows the curve latitude = −80 sin(solar longitude), with deviations. We find that the peak brightness is 5 ± 4.5 kR, situated at 72 ± 10.4 km. It ranges from 0.23 to 18.51 kR and from 42 to 97 km. These values are consistent with previous studies. We also present maps of the brightness of the NO emission peak and its variability, an important factor that can reach up to 50% of the emission and is not reproduced by average brightness model maps. The characteristics and factors that may control the emission are investigated. In particular, we show that the solar activity exerts a positive influence on the number of detections. It does not influence, on the contrary, the brightness or altitude of the peak of the NO nightglow emission. Results presented in this study lead to future comparisons with global Martian atmospheric models and observational targets for the Imaging Ultraviolet Sprectrograph Mars Atmosphere and Volatile Evolution.
We present direct number density retrievals of carbon dioxide (CO2) and molecular nitrogen (N2) for the upper atmosphere of Mars using limb scan observations during October and November 2014 by the Imaging Ultraviolet Spectrograph on board NASA's Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft. We use retrieved CO2 densities to derive temperature variability between 170 and 220 km. Analysis of the data shows (1) low‐mid latitude northern hemisphere CO2 densities at 170 km vary by a factor of about 2.5, (2) on average, the N2/CO2 increases from 0.042 ± 0.017 at 130 km to 0.12 ± 0.06 at 200 km, and (3) the mean upper atmospheric temperature is 324 ± 22 K for local times near 14:00.
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