The infrared spectrum of the matrix-isolated phenyl radical

被引:99
作者
Friderichsen, AV
Radziszewski, JG
Nimlos, MR
Winter, PR
Dayton, DC
David, DE
Ellison, GB
机构
[1] Natl Renewable Energy Lab, Golden, CO 80401 USA
[2] Univ Colorado, Dept Chem & Biochem, Boulder, CO 80309 USA
[3] Univ Colorado, CIRES, Integrated Instrument Design Facil, Boulder, CO 80309 USA
[4] Colorado Sch Mines, Dept Chem Engn & Petr Refining, Golden, CO 80401 USA
关键词
D O I
10.1021/ja0024338
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We have measured the infrared absorption spectrum of C6H5, (X) over tilde (2)A(1), in an Ar matrix at 10 K. The experimental frequencies (cm(-1)) and polarizations follow, a(1) modes: 3086; 3072, 3037, 1581, 1441, 1154, 1027, 997, 976, 605;b(1) modes: 972, 874, 706, 657, 416; b(2) modes: 3071, 3069, 1624, 1432, 1321, 1283, 1 159, 1063, and 587. Three different methods have been used for the production of the phenyl radicals. Infrared absorption spectra of five deuterated isotopomers, C6D5, p-C6H4D, p-C6HD4, o-C6H4D, and m-C6H4D, were recorded to compare experimental frequency shifts with calculated (UB3LYP/cc-pVDZ) harmonic frequency shifts. The use of CO2 or NO as internal standards enabled the experimental determination of absolute infrared intensities. The linear dichroism was measured with photooriented samples to establish experimental polarizations of each vibrational band. True gas-phase vibrational frequencies were estimated by considering the gas-to-matrix shifts and matrix;inhomogeneous line broadening. The phenyl radical matrix frequencies listed above are within +/-1% of the gas-phase vibrational frequencies. The C6H5 frequencies from this paper supersede our earlier values reported in J. Am. Chem. Soc. 1996, 118, 7400-7401.
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页码:1977 / 1988
页数:12
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