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首页> 外文期刊>The Journal of Chemical Physics >Rotational constants and structure of para-difluorobenzene determined by femtosecond Raman coherence spectroscopy: A new transient type
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Rotational constants and structure of para-difluorobenzene determined by femtosecond Raman coherence spectroscopy: A new transient type

机译:飞秒拉曼相干光谱法测定对二氟苯的旋转常数和结构:一种新型的瞬态类型

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Femtosecond Raman rotational coherence spectroscopy (RCS) detected by degenerate four-wave mixing is a background-free method that allows to determine accurate gas-phase rotational constants of non-polar molecules. Raman RCS has so far mostly been applied to the regular coherence patterns of symmetric-top molecules, while its application to nonpolar asymmetric tops has been hampered by the large number of RCS transient types, the resulting variability of the RCS patterns, and the 10(3)-10(4) times larger computational effort to simulate and fit rotational Raman RCS transients. We present the rotational Raman RCS spectra of the nonpolar asymmetric top 1,4-difluorobenzene (para-difluorobenzene, p-DFB) measured in a pulsed Ar supersonic jet and in a gas cell over delay times up to similar to 2.5 ns. p-DFB exhibits rotational Raman transitions with Delta J = 0,1,2 and Delta K = 0, 2, leading to the observation of J-, K-, A-, and C-type transients, as well as a novel transient (S-type) that has not been characterized so far. The jet and gas cell RCS measurements were fully analyzed and yield the ground-state (v = 0) rotational constants A(0) = 5637.68(20) MHz, B-0 = 1428.23(37) MHz, and C-0 = 1138.90(48) MHz (1 sigma uncertainties). Combining the A(0), B-0, and C-0 constants with coupled-cluster with single-, double-and perturbatively corrected triple-excitation calculations using large basis sets allows to determine the semi-experimental equilibrium bond lengths r(e)(C-1-C-2) = 1.3849(4) angstrom, r(e)(C-2-C-3) = 1.3917(4) angstrom, r(e)(C-F) = 1.3422(3) angstrom, and r(e)(C-2-H-2) = 1.0791(5) angstrom. (C) 2015 AIP Publishing LLC.
机译:通过简并四波混合检测的飞秒拉曼旋转相干光谱(RCS)是无背景方法,可用于确定非极性分子的精确气相旋转常数。迄今为止,拉曼RCS大部分已应用于对称顶分子的规则相干图案,而其在非极性非对称顶上的应用却受到大量RCS瞬态类型,RCS图案的最终变异性以及10( 3)-10(4)乘以较大的计算量来模拟和拟合旋转拉曼RCS瞬变。我们介绍了在脉冲Ar超音速射流和气室中,在长达约2.5 ns的延迟时间内测量的非极性不对称顶部1,4-二氟苯(对二氟苯,p-DFB)的旋转拉曼RCS光谱。 p-DFB表现出旋转拉曼跃迁,ΔJ = 0,1,2,ΔK = 0,2,导致观察到J型,K型,A型和C型瞬态,以及一种新颖的瞬态(S型)到目前为止尚未表征。对射流和气室RCS测量进行了全面分析,得出基态(v = 0)旋转常数A(0)= 5637.68(20)MHz,B-0 = 1428.23(37)MHz和C-0 = 1138.90 (48)MHz(不确定的1 sigma)。将A(0),B-0和C-0常数与耦合簇结合起来,并使用大基集进行单次,两次和微扰校正的三次激发计算,从而可以确定半实验平衡键长度r(e )(C-1-C-2)= 1.3849(4)埃,r(e)(C-2-C-3)= 1.3917(4)埃,r(e)(CF)= 1.3422(3)埃,而r(e)(C-2-H-2)= 1.0791(5)埃。 (C)2015 AIP Publishing LLC。

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