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arXiv 1712.04486astro-ph.EP
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土卫六大气2 μm窗口的透明度

Transparency of 2 μm window of Titan's atmosphere

Pascal Rannou, Benoît Seignovert, Stéphane Le Mouélic, Lucas Maltagliati, Micheal Rey, Christophe Sotin

摘要:

土卫六的大气层在光学上很厚,几乎在所有波长下都看不到它的表面和下层。然而,由于气体反射是光谱选择性的,一些窄的光谱间隔是相对透明的,并允许探测表面。为了使用这些间隔(称为窗口),必须充分了解大气吸收。一旦气体光谱线列很好地建立,窗口内的吸收取决于甲烷吸收线的远翼被切断的方式。我们知道,除了2 μm窗口外,所有窗口中的强度都可以用相同的截止参数来解释。这种差异通常采用一种变通方法来处理,即对该特定窗口使用不同的截止值描述。该窗口相对透明,并且表面可以具有可以被检测到的特定光谱特征。因此,对大气不透明度的良好了解是必不可少的,我们的范围是更好地理解是什么导致了2 μm窗口和其他窗口之间的差异。在这项工作中,我们使用的散射光在肢体和传输掩星观测与VIMS(视觉红外测绘光谱仪)卡西尼号上,周围的2 μm窗口。数据显示了参与该窗口形状的吸收特征。我们的大气模型与2 μm处的VIMS数据拟合得很好,与其他窗口相比具有相同的截止值,前提是在约2.065 μm的窗口中间引入额外的吸收。它很好地解释了在2 μm处使用的截止值之间的差异,并且我们表明具有相当恒定的混合比的气体(可能是乙烷)可能是这种吸收的原因。最后,我们研究了这种吸收对地表反射率反演的影响,发现它是显着的。

英文摘要:

Titan's atmosphere is optically thick and hides the surface and the lower layers from the view at almost all wavelengths. However, because gaseous absorptions are spectrally selective, some narrow spectral intervals are relatively transparent and allow to probe the surface. To use these intervals (called windows) a good knowledge of atmospheric absorption is necessary. Once gas spectroscopic linelists are well established, the absorption inside windows depends on the way the far wings of the methane absorption lines are cut-off. We know that the intensity in all the windows can be explained with the same cut-off parameters, except for the window at 2 μm. This discrepancy is generally treated with a workaround which consists in using a different cut-off description for this specific window. This window is relatively transparent and surface may have specific spectral signatures that could be detected. Thus, a good knowledge of atmosphere opacities is essential and our scope is to better understand what causes the difference between the 2 μm window and the other windows. In this work, we used scattered light at the limb and transmissions in occultation observed with VIMS (Visual Infrared Mapping Spectrometer) onboard Cassini, around the 2 μm window. Data shows an absorption feature that participates to the shape of this window. Our atmospheric model fits well the VIMS data at 2 μm with the same cut-off than for the other windows, provided an additional absorption is introduced in the middle of the window around ~2.065 μm. It explains well the discrepancy between the cut-off used at 2 μm, and we show that a gas with a fairly constant mixing ratio, possibly ethane, may be the cause of this absorption. Finally, we studied the impact of this absorption on the retrieval of the surface reflectivity and found that it is significant.

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