首页> 外文期刊>Icarus: International Journal of Solar System Studies >The application of new methane line absorption data to Gemini-N/NIFS and KPNO/FTS observations of Uranus' near-infrared spectrum
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The application of new methane line absorption data to Gemini-N/NIFS and KPNO/FTS observations of Uranus' near-infrared spectrum

机译:新的甲烷谱线吸收数据在天王星近红外光谱的Gemini-N / NIFS和KPNO / FTS观测中的应用

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New line data describing the absorption of CH _4 and CH _3D from 1.26 to 1.71μm (Campargue, A., Wang, L., Mondelain, D., Kassi, S., Bézard, B., Lellouch, E., Coustenis, A., de Bergh, C., Hirtzig, M., Drossart, P. [2012]. Icarus 219, 110-128), building upon previous papers by Campargue et al. (Campargue, A., Wang, L., Kassi, S., Masat, M., Votava, O. [2010]. J. Quant. Spectrosc. Radiat. Transfer 111, 1141-1151; Wang, L., Kassi, S., Campargue, A. [2010]. J. Quant. Spectrosc. Radiat. Transfer 111, 1130-1140; Wang, L., Kassi, S., Liu, A.W., Hu, S.M., Campargue, A. [2011]. J. Quant. Spectrosc. Radiat. Transfer 112, 937-951)) have been applied to the analysis of Gemini-N/NIFS observations of Uranus made in 2010 and compared with earlier disc-averaged observations made by KPNO/FTS in 1982. The new line data are found to improve greatly the fit to the observed spectra and present a huge advance over previous methane absorption tables by allowing us to determine the CH _3D/CH _4 ratio and also start to break the degeneracy between methane abundance and cloud top height. The best fits are obtained if the cloud particles in the main cloud deck at the 2-3bar level become less scattering with wavelength across the 1.4-1.6μm region and we have modelled this variation here by varying the extinction cross-section and single-scattering albedo of the particles.Applying the new line data to the NIFS spectra of Uranus, we determine a new estimate of the CH _3D/CH _4 ratio of 2.9-0.5+0.9×10-4, which is consistent with the estimate of de Bergh et al. (de Bergh, C., Lutz, B.L., Owen, T., Brault, J., Chauville, J. [1986]. Astrophys. J. 311, 501-510) of 3.6-2.8+3.6×10-4, made by fitting a disc-averaged KPNO/FTS spectrum measured in 1982, but much better constrained. The NIFS observations made in 2010 have been disc-averaged and compared with the 1982 KPNO/FTS spectrum and found to be in excellent agreement.Using k-tables fitted to the new line data, the central meridian observations of Uranus' H-band spectrum (1.49-1.64μm) made by Gemini-N/NIFS in 2010 have been reanalyzed. The use of the new methane absorption coefficients and the modified scattering properties of the cloud particles in the main cloud deck appears to break the degeneracy between cloud height and methane abundance immediately above it in this spectral region and we find that both vary with latitude across Uranus' disc. Overall, we find that the main cloud deck becomes higher, but thinner from equator to poles, with a local maximum in cloud top height in the circumpolar zones at 45°N and 45°S. At the same time, using the 'D' temperature pressure profile of Lindal et al. (Lindal, G.F., Lyons, J.R., Sweetnam, D.N., Eshleman, V.R., Hinson, D.P. [1987]. J. Geophys. Res. 92, 14987-15001) and a deep methane abundance of 1.6% (Baines, K.H., Mickelson, M.E., Larson, L.E., Ferguson, D.W. [1995]. Icarus 144, 328-340) we find that the relative humidity of methane is high near the equator (~60%) and decreases sharply towards the poles, except near the circumpolar zone at 45°N, which has brightened steadily since 2007, and where there is a local maximum in methane relative humidity. In tests conducted with the warmer 'F1' profile of Sromovsky et al. (2011) we find a similar variation of methane abundance above the main cloud, although for this warmer temperature profile this abundance is dependent mostly on the fitted deep methane mole fraction.
机译:换行数据描述了CH _4和CH _3D在1.26至1.71μm的吸收(Campargue,A.,Wang,L.,Mondelain,D.,Kassi,S.,Bézard,B.,Lellouch,E.,Coustenis, A.,de Bergh,C.,Hirtzig,M.,Drossart,P. [2012]。Icarus 219,110-128),基于Campargue等人先前的论文。 (Campargue,A.,Wang,L.,Kassi,S.,Masat,M.,Votava,O. [2010]。J. Quant。Spectrosc.Radiat.Transfer 111,1141-1151; Wang,L.,Kassi ,S.,Campargue,A. [2010]。J. Quant。Spectrosc。Radiat。Transfer 111,1130-1140; Wang,L.,Kassi,S.,Liu,AW,Hu,SM,Campargue,A. [ 2011]。J. Quant。Spectrosc。Radiat。Transfer 112,937-951))已用于分析2010年对天王星的Gemini-N / NIFS观测结果,并与KPNO / FTS先前的盘均观测值进行了比较1982年。发现了新的谱线数据后,我们可以确定CH _3D / CH _4的比值,也开始打破甲烷丰度之间的简并性,大大提高了对观测光谱的拟合度,并比以前的甲烷吸收表有了巨大的进步。和云顶高度。如果在2-3bar高度的主云层中的云颗粒在1.4-1.6μm区域内的波长处的散射变得更少,则将获得最佳拟合,并且我们通过改变消光截面和单散射在此模拟了这种变化将新的线数据应用于天王星的NIFS光谱,我们确定CH _3D / CH _4比值的新估计为2.9-0.5 + 0.9×10-4,这与de Bergh的估计一致等。 (de Bergh,C.,Lutz,BL,Owen,T.,Brault,J.,Chauville,J. [1986]。Astrophys。J. 311,501-510)为3.6-2.8 + 3.6×10-4,通过拟合1982年测得的圆盘平均KPNO / FTS谱而制得,但受到的约束要好得多。对2010年的NIFS观测值进行了盘平均,并与1982年的KPNO / FTS谱进行了比较,发现它们之间具有很好的一致性。使用适合新线数据的k表,天王星H谱带的中央子午线观测重新分析了Gemini-N / NIFS在2010年制造的(1.49-1.64μm)。使用新的甲烷吸收系数和修改后的主云层中云颗粒的散射特性似乎打破了该光谱区域中云层高度和紧接其上方的甲烷丰度之间的退化,我们发现两者在天王星上均随纬度而变化光盘。总体而言,我们发现主云层变得更高,但从赤道到两极都变薄,在45°N和45°S的绕极区云顶高度局部最高。同时,使用Lindal等人的“ D”温度压力曲线。 (Lindal,GF,Lyons,JR,Sweetnam,DN,Eshleman,VR,Hinson,DP [1987]。J. Geophys。Res。92,14987-15001)和1.6%的深甲烷丰度(Baines,KH,Mickelson) ,ME,Larson,LE,Ferguson,DW [1995]。Icarus 144,328-340),我们发现甲烷的相对湿度在赤道附近较高(约60%),并向两极急剧下降,除非在极地附近。该区域位于45°N,自2007年以来一直稳定增亮,甲烷相对湿度局部最高。在用Sromovsky等人的“ F1”变暖曲线进行的测试中。 (2011年),我们在主云之上发现了类似的甲烷丰度变化,尽管对于较暖的温度曲线,该丰度主要取决于拟合的深层甲烷摩尔分数。

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