首页> 外文期刊>The Journal of Chemical Physics >Rotational spectrum and carbon-13 hyperfine structure of the C3H, C5H, C6H, and C7H radicals
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Rotational spectrum and carbon-13 hyperfine structure of the C3H, C5H, C6H, and C7H radicals

机译:C3H,C5H,C6H和C7H自由基的旋转光谱和碳13超细结构

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By means of Fourier transform microwave spectroscopy of a supersonic molecular beam, we have detected the singly substituted carbon-13 isotopic species of C5H, C6H, and C7H. Hyperfine structure in the rotational transitions of the lowest-energy fine structure component ((2)Pi(1/2) for C5H and C7H, and (2)Pi(3/2) for C6H) of each species was measured between 6 and 22 GHz, and precise rotational, centrifugal distortion, Lambda-doubling, and C-13 hyperfine coupling constants were determined. In addition, resolved hyperfine structure in the lowest rotational transition (J=3/2 -> 1/2) of the three C-13 isotopic species of C3H was measured by the same technique. By combining the centimeter-wave measurements here with previous millimeter-wave data, a complete set of C-13 hyperfine coupling constants were derived to high precision for each isotopic species. Experimental structures (r(0)) have been determined for C5H and the two longer carbon-chain radicals, and these are found to be in good agreement with the predictions of high-level coupled-cluster calculations. C3H, C5H, and C7H exhibit a clear alternation in the magnitude and sign of the C-13 hyperfine coupling constants along the carbon-chain backbone. Because the electron spin density is nominally zero at the central carbon atom of C3H, C5H, and C7H, and at alternating sets of carbon atoms of C5H and C7H, owing to spin polarization, almost all of the C-13 coupling constants at these atoms are small in magnitude and negative in sign. Spin-polarization effects are known to be important for the Fermi-contact (b(F)) term, but prior to the work here they have generally been neglected for the hyperfine terms a, c, and d. (c) 2005 American Institute of Physics.
机译:通过超音速分子束的傅立叶变换微波光谱,我们已经检测到C5H,C6H和C7H的单取代碳13同位素物种。测量了每个物种的最低能量精细结构成分(C5H和C7H为(2)Pi(1/2)和C6H为(2)Pi(3/2))的旋转跃迁中的超精细结构。确定了22 GHz的频率,并确定了精确的旋转,离心失真,λ加倍和C-13超精细耦合常数。另外,通过相同技术测量了C 3 H的三个C-13同位素物种的最低旋转跃迁(J = 3/2-> 1/2)中的分解的超精细结构。通过将此处的厘米波测量值与先前的毫米波数据相结合,可以为每种同位素物种高精度地导出一整套C-13超精细耦合常数。实验结构(r(0))已确定为C5H和两个较长的碳链自由基,并且与高级耦合簇计算的预测相符。 C3H,C5H和C7H在沿碳链主链的C-13超精细偶合常数的大小和符号上表现出明显的交替。由于自旋极化,由于C3H,C5H和C7H的中心碳原子以及C5H和C7H的交替碳原子组的电子自旋密度名义上为零,因此在这些原子上几乎所有的C-13耦合常数幅度较小,符号为负。众所周知,自旋极化效应对于费米接触(b(F))项很重要,但是在此进行工作之前,通常对于超精细项a,c和d忽略了它们。 (c)2005年美国物理研究所。

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