Selby Talitha M, Clarkson Jasper R, Mitchell Diane, Fitzpatrick James A J, Lee Hsiupu D, Pratt David W, Zwier Timothy S
Department of Chemistry, Purdue University, West Lafayette, Indiana 47907-2084, USA.
J Phys Chem A. 2005 May 26;109(20):4484-96. doi: 10.1021/jp050858g.
The infrared and ultraviolet spectroscopy of o-, m-, and p-ethynylstyrene isomers (oES, mES, and pES) were studied by a combination of methods, including resonance-enhanced two-photon ionization (R2PI), UV-UV hole-burning spectroscopy (UVHB), resonant ion-dip infrared spectroscopy (RIDIRS), and rotationally resolved fluorescence excitation spectroscopy. In addition, the newly developed method of stimulated emission pumping-population transfer spectroscopy (SEP-PTS) was used to determine the energy threshold to conformational isomerization in m-ethynylstyrene. The S(1) <-- S(0) origin transitions of oES and pES occur at 32 369 and 33 407 cm(-1), respectively. In mES, the cis and trans conformations are calculated to be close in energy. In the R2PI spectrum of mES, the two most prominent peaks (32672 and 32926 cm(-1)) were confirmed by UVHB spectroscopy to be S(1) <-- S(0) origins of these two conformers. The red-shifted conformer was identified as the cis structure by least-squares fitting of the rotationally resolved fluorescence excitation spectrum of the origin band. There are also two possible conformations in oES, but transitions due to only one were observed experimentally, as confirmed by UVHB spectroscopy. Density functional theory calculations (B3LYP/6-31+G) predict that the cis-ortho conformer, in which the substituents point toward each other, is about 8 kJ/mol higher in energy than the trans-ortho isomer, and should only be about 5% of the room temperature population of oES. Ground-state infrared spectra in the C-H stretch region (3000-3300 cm(-1)) of each isomer were obtained with RIDIRS. In all three structural isomers, the acetylenic C-H stretch fundamental was split by Fermi resonance. Infrared spectra were also recorded in the excited electronic state, using a UV-IR-UV version of RIDIR spectroscopy. In all three isomers the acetylenic C-H stretch fundamental was unshifted from the ground state, but no Fermi resonance was seen. The first observed and last unobserved transitions in the SEP-PT spectrum were used to place lower and upper bounds on the barrier to cis --> trans isomerization in m-ethynylstyrene of 990-1070 cm(-1). Arguments are given for the lack of a kinetic shift in the measurement. The analogous trans --> cis barrier is in the same range (989-1065 cm(-1)), indicating that the relative energies of the zero-point levels of the two isomers are (E(ZPL)(cis) - E(ZPL)(trans))= -75 to +81 cm(-1). Both the barrier heights and relative energies of the minima are close to those determined by DFT (Becke3LYP/6-31+G) calculations.
通过多种方法相结合,包括共振增强双光子电离(R2PI)、紫外 - 紫外空穴烧蚀光谱(UVHB)、共振离子偶极红外光谱(RIDIRS)和转动分辨荧光激发光谱,研究了邻位、间位和对位乙炔基苯乙烯异构体(oES、mES和pES)的红外和紫外光谱。此外,还使用了新开发的受激发射泵浦 - 布居转移光谱(SEP - PTS)方法来确定间位乙炔基苯乙烯构象异构化的能量阈值。oES和pES的S(1)←S(0)起始跃迁分别发生在32369和33407 cm⁻¹处。在mES中,顺式和反式构象经计算能量相近。在mES的R2PI光谱中,UVHB光谱证实两个最突出的峰(32672和32926 cm⁻¹)分别是这两种构象的S(1)←S(0)起始峰。通过对起始带的转动分辨荧光激发光谱进行最小二乘拟合,确定红移构象为顺式结构。oES中也存在两种可能的构象,但通过UVHB光谱证实,实验上仅观察到了其中一种构象的跃迁。密度泛函理论计算(B3LYP/6 - 31 + G)预测,取代基相互指向的顺式邻位构象比反式邻位异构体能量高约8 kJ/mol,且在oES的室温布居中所占比例仅约为5%。使用RIDIRS获得了各异构体在C - H伸缩振动区域(3000 - 3300 cm⁻¹)的基态红外光谱。在所有三种结构异构体中,炔基C - H伸缩振动基频因费米共振而分裂。还使用RIDIR光谱的紫外 - 红外 - 紫外版本记录了激发电子态的红外光谱。在所有三种异构体中,炔基C - H伸缩振动基频相对于基态未发生位移,但未观察到费米共振。SEP - PT光谱中首次观察到的跃迁和最后未观察到的跃迁用于确定间位乙炔基苯乙烯顺式→反式异构化势垒的下限和上限,范围为990 - 1070 cm⁻¹。文中给出了测量中不存在动力学位移的论据。类似的反式→顺式势垒在相同范围内(989 - 1065 cm⁻¹),表明两种异构体零点能的相对能量为(E(ZPL)(顺式) - E(ZPL)(反式))= -75至 +81 cm⁻¹。势垒高度和极小值的相对能量均与DFT(Becke三LYP/6 - 31 + G)计算结果相近。