乙酰胺的第三激发态

V. Ilyushin, R. Porohovoi, E. Alekseev, M. Pogrebnyak, H. Müller, F. Lewen, S. Schlemmer
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引用次数: 0

摘要

我们提出了我们对乙酰胺分子CH3CONH2的扭旋光谱的新研究结果。尽管在星际介质中发现了相当丰富的乙酰胺,但迄今为止对其旋转光谱的研究仅达到$J_{\max}=20$。本研究的目的是扩展分析中涉及的量子数范围(从而提高对高激发态的预测质量)以及频率范围覆盖。新的测量是从毫米波范围(从34.5 GHz开始)到亚毫米波范围(高达645 GHz),使用哈尔科夫和Köln实验室的光谱仪进行的。我们对$J_{\max}=62$时乙酰胺$v_{\ mathm {t}}=0,1,2$扭转态的初步拟合揭示了一些扰动,我们将其归因于由NH2在~ 259 cm−1的摆动状态引起的扭曲(通过扭间相互作用向下传播到低处的扭转态)。将我们的任务扩展到乙酰胺的第三激发态是明确解释与乙酰胺的NH2摆动态相互作用的准备步骤。到目前为止,共有421个a型和263个J=32的e型旋转跃迁属于乙酰胺的第三激扭态。使用rho轴方法拟合包含8240个旋转转换的联合$v_{\ mathm {t}}=0,1,2,3$数据集,对包含114个参数的哈密顿模型给出加权均方根偏差2.8。
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The Third Excited Torsional State of Acetamide
We present the results of our new study of the torsion-rotation spectrum of the acetamide molecule, CH3CONH2. Despite the fact that acetamide was found to be quite abundant in the interstellar medium, its rotation spectrum was studied only up to $J_{\max}=20$ so far. The aim of the present study was to extend the quantum number range involved in the analysis (thus improving the quality of predictions for higher excited rotational states) as well as the frequency range coverage. The new measurements were carried out from the millimeter wave range (starting at 34.5 GHz) to the sub-millimeter wave range (up to 645 GHz) using spectrometers in the Kharkiv and Köln laboratories. Our preliminary fits of the $v_{\mathrm{t}}=0,1,2$ torsional states of acetamide with $J_{\max}=62$ revealed some perturbations, which we attribute to distortions caused by the NH2 wagging state at ∼259 cm−1 (that propagate down to low-lying torsional states via intertorsional interactions). The extension of our assignments to the third excited torsional state of acetamide is a preparatory step toward explicitly accounting for interactions with the NH2 wagging state of acetamide. So far, 421 A-type and 263 E-type rotational transitions up to $J=32$ belonging to the third excited torsional state of acetamide were assigned and added to the analysis. A joint $v_{\mathrm{t}}=0,1,2,3$ dataset involving 8240 rotational transitions was fit using the rho axis method giving a weighted root mean square deviation of 2.8 for a Hamiltonian model that includes 114 parameters.
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