arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1502.06867astro-ph.GAastro-ph.EPphysics.atm-clusphysics.chem-ph
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用转动光谱研究对称顶层分子中振动多面体间的相互作用:甲基氰的低激发态$v_8 \le 2$,CH $_3$ CN

Rotational spectroscopy as a tool to investigate interactions between vibrational polyads in symmetric top molecules: low-lying states $v_8 \le 2$ of methyl cyanide, CH$_3$CN

Holger S. P. Müller, Linda R. Brown, Brian J. Drouin, John C. Pearson, Isabelle Kleiner, Robert L. Sams, Keeyoon Sung, Matthias H. Ordu, Frank Lewen

摘要:

记录乙腈的光谱是为了分析低振动态的相互作用,并为射电天文观测和行星大气的红外光谱研究构建谱线列表。旋转光谱覆盖了36 $-$ 1627 GHz区域的大部分。在红外(IR)中,在717 cm $^{-1}$周围的2 $ν_8$区域中记录了本研究的光谱,其分配覆盖684 $-$ 765 cm $^{-1}$。使用$ν_8$区域中的其他光谱来验证分析。大量和高精度的旋转数据扩展到更高的$J$和$K$量子数,使我们能够第一次深入研究这些状态之间的局部相互作用,这些状态发生在高$K$值。特别是,我们已经检测到$v_8 = 1$和2之间的几个相互作用。值得注意的是,在$K$ = 14时,在$v_8 = 1^{-1}$和$v_8 = 2^{+2}$之间存在强的$Δv_8 = \pm1$、$ΔK = 0$、$Δl = \pm3$费米共振。光谱中的显著效应也是由$v_8 = 1$和2之间的共振$Δv_8 = \pm1$、$ΔK = \mp2$、$Δl = \pm1$相互作用引起的。在基态的$K$ = 14和$v_8 = 1$的$K$ = 12,$l = +1$之间发生了一种等效的共振相互作用,我们首次对此作了详细的解释.在较早的研究中对基态振动态作了初步的说明。从有关$v_8 = 2$的数据,我们还研究了与$v_4 = 1$的旋转相互作用以及$v_8 = 2$和3之间的$Δv_8 = \pm1$,$ΔK = 0$,$Δl = \pm3$费米相互作用。我们已经推导出N $_2$和自增宽系数的$ν_8$,2 $ν_8 - ν_8$,和2 $ν_8$频带从先前确定的nu4值。随后,我们确定了三个红外波段的跃迁矩和强度。

英文摘要:

Spectra of methyl cyanide were recorded to analyze interactions in low-lying vibrational states and to construct line lists for radio astronomical observations as well as for infrared spectroscopic investigations of planetary atmospheres. The rotational spectra cover large portions of the 36$-$1627 GHz region. In the infrared (IR), a spectrum was recorded for this study in the region of 2$ν_8$ around 717 cm$^{-1}$ with assignments covering 684$-$765 cm$^{-1}$. Additional spectra in the $ν_8$ region were used to validate the analysis. The large amount and the high accuracy of the rotational data extend to much higher $J$ and $K$ quantum numbers and allowed us to investigate for the first time in depth local interactions between these states which occur at high $K$ values. In particular, we have detected several interactions between $v_8 = 1$ and 2. Notably, there is a strong $Δv_8 = \pm1$, $ΔK = 0$, $Δl = \pm3$ Fermi resonance between $v_8 = 1^{-1}$ and $v_8 = 2^{+2}$ at $K$ = 14. Pronounced effects in the spectrum are also caused by resonant $Δv_8 = \pm1$, $ΔK = \mp2$, $Δl = \pm1$ interactions between $v_8 = 1$ and 2. An equivalent resonant interaction occurs between $K$ = 14 of the ground vibrational state and $K$ = 12, $l = +1$ of $v_8 = 1$ for which we present the first detailed account. A preliminary account was given in an earlier study on the ground vibrational state. From data pertaining to $v_8 = 2$, we also investigated rotational interactions with $v_4 = 1$ as well as $Δv_8 = \pm1$, $ΔK = 0$, $Δl = \pm3$ Fermi interactions between $v_8 = 2$ and 3. We have derived N$_2$- and self-broadening coefficients for the $ν_8$, 2$ν_8 - ν_8$, and 2$ν_8$ bands from previously determined nu4 values. Subsequently, we determined transition moments and intensities for the three IR bands.

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