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首页> 外文期刊>Annales Geophysicae >A comparison of ground-based hydroxyl airglow temperatures with SABER/TIMED measurements over 23 degrees N, India
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A comparison of ground-based hydroxyl airglow temperatures with SABER/TIMED measurements over 23 degrees N, India

机译:比较印度23°N以上地面温度和SABER / TIMED的地面羟基气辉剂温度

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Ground-based observations of OH(6, 2) Meinel band nightglow were carried out at Ranchi (23.3 degrees N, 85.3 degrees E), India, during January-March 2011, December 2011-May 2012 and December 2012-March 2013 using an all-sky imaging system. Near the mesopause, OH temperatures were derived from the OH(6, 2) Meinel band intensity information. A limited comparison of OH temperatures (T-OH) with SABER/TIMED measurements in 30 cases was performed by defining almost coincident criterion of +/- 1.5 degrees latitude-longitude and +/- 3 min of the ground-based observations. Using SABER OH 1.6 and 2.0 mu m volume emission rate profiles as the weighing function, two sets of OH-equivalent temperature (T-1.6 and T-2.0 respectively) were estimated from its kinetic temperature profile for comparison with OH nightglow measurements. Overall, fair agreement existed between ground-based and SABER measurements in the majority of events within the limits of experimental errors. Overall, the mean value of OH-derived temperatures and SABER OH-equivalent temperatures were 197.3 +/- 4.6, 192.0 +/- 10.8 and 192.7 +/- 10.3 K, and the ground-based temperatures were 4-5K warmer than SABER values. A difference of 8K or more is noted between two measurements when the peak of the OH emission layer lies in the vicinity of large temperature inversions. A comparison of OH temperatures derived using different sets of Einstein transition probabilities and SABER measurements was also performed; however, OH temperatures derived using Langhoff et al. (1986) transition probabilities were found to compare well.
机译:在2011年1月至2011年3月,2011年12月至2012年5月以及2012年12月至2013年3月期间,在印度兰契(北23.3度,东85.3度)对OH(6,2)Meinel带夜光进行了地面观测。全天候成像系统。在中绝经期附近,OH温度是从OH(6,2)Meinel带强度信息得出的。通过定义纬度+/- 1.5度和地面观测值+/- 3分钟的几乎一致的标准,对OH温度(T-OH)与SABER / TIMED测量在30个案例中进行了有限的比较。使用SABER OH 1.6和2.0μm体积排放速率曲线作为称量函数,从其动力学温度曲线中估算出两组OH等效温度(分别为T-1.6和T-2.0),以与OH夜光测量进行比较。总体而言,在大多数情况下,在实验误差范围内,地面和SABER测量之间存在公平的协议。总体而言,OH衍生温度和SABER OH等效温度的平均值分别为197.3 +/- 4.6、192.0 +/- 10.8和192.7 +/- 10.3 K,地面温度比SABER值高4-5K 。当OH发射层的峰值位于大的温度反转附近时,两次测量之间会发现8K或更大的差异。还比较了使用不同组爱因斯坦跃迁概率和SABER测量得出的OH温度;但是,使用Langhoff等人得出的OH温度。 (1986)发现过渡概率比较好。

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