Blake Thomas A, Glendening Eric D, Sams Robert L, Sharpe Steven W, Xantheas Sotiris S
Chemical and Materials Sciences Division, Pacific Northwest National Laboratory, P.O. Box 999, MS K8-88, Richland, Washington 99352, USA.
J Phys Chem A. 2007 Nov 8;111(44):11328-41. doi: 10.1021/jp072521f. Epub 2007 Jul 6.
We present experimental infrared spectra and theoretical electronic structure results for the geometry, anharmonic vibrational frequencies, and accurate estimates of the magnitude and the origin of the ring-puckering barrier in C4F8. High-resolution (0.0015 cm-1) spectra of the nu12 and nu13 parallel bands of perfluorocyclobutane (c-C4F8) were recorded for the first time by expanding a 10% c-C4F8 in helium mixture in a supersonic jet. Both bands are observed to be rotationally resolved in a jet with a rotational temperature of 15 K. The nu12 mode has b2 symmetry under D2d that correlates to a2u symmetry under D4h and consequently has +/- <-- +/- ring-puckering selection rules. A rigid rotor fit of the nu12 band yields the origin at 1292.56031(2) cm-1 with B' = 0.0354137(3) cm-1 and B' ' = 0.0354363(3) cm-1. The nu13 mode is of b2 symmetry under D2d that correlates to b2g under D4h, and in this case, the ring-puckering selection rules are +/- <-- -/+ . Rotational transitions from the ground and first excited torsional states will be separated by the torsional splitting in the ground and excited vibrational states, and indeed, we observe a splitting of each transition into strong and weak intensity components with a separation of approximately 0.0018 cm-1. The strong and weak sets of transitions were fit separately again using a rigid rotor model to give nu13(strong) = 1240.34858(4) cm-1, B' = 0.0354192(7) cm-1, and B' ' = 0.0354355(7) cm-1 and nu13(weak) = 1240.34674(5) cm-1, B' = 0.0354188(9) cm-1, and B' ' = 0.0354360(7) cm-1. High-level electronic structure calculations at the MP2 and CCSD(T) levels of theory with the family of correlation consistent basis sets of quadruple-zeta quality, developed by Dunning and co-workers, yield best estimates for the vibrationally averaged structural parameters r(C-C) = 1.568 A, r(C-F)alpha = 1.340 A, r(C-F)beta = 1.329 A, alpha(F-C-F) = 110.3 degrees , thetaz(C-C-C) = 89.1 degrees , and delta(C-C-C-C) = 14.6 degrees and rotational constants of A = B = 0.03543 cm-1 and C = 0.02898 cm-1, the latter within 0.00002 cm-1 from the experimentally determined values. Anharmonic vibrational frequencies computed using higher energy derivatives at the MP2 level of theory are all within <27 cm-1 (in most cases <5 cm-1) from the experimentally measured fundamentals. Our best estimate for the ring-puckering barrier at the CCSD(T)/CBS (complete basis set) limit is 132 cm-1. Analysis of the C4F8 electron density suggests that the puckering barrier arises principally from the sigmaCC-->sigmaCF hyperconjugative interactions that are more strongly stabilizing in the puckered than in the planar form. These interactions are, however, somewhat weaker in C4F8 than in C4H8, a fact that is consistent with the smaller barrier in the former (132 cm-1) with respect to the latter (498 cm-1).
我们给出了全氟环丁烷(C4F8)的几何结构、非谐振动频率以及环面翻转势垒大小和来源的精确估计的实验红外光谱和理论电子结构结果。通过在超声速射流中膨胀10%的C4F8与氦气的混合物,首次记录了全氟环丁烷(c-C4F8)的ν12和ν13平行带的高分辨率(0.0015 cm-1)光谱。在旋转温度为15 K的射流中,观察到这两个带都具有旋转分辨。ν12模式在D2d点群下具有b2对称性,在D4h点群下与a2u对称性相关,因此具有+/- <-- +/-的环面翻转选择规则。对ν12带进行刚性转子拟合,得到其谱带起源为1292.56031(2) cm-1,B' = 0.0354137(3) cm-1,B'' = 0.0354363(3) cm-1。ν13模式在D2d点群下为b2对称性,在D4h点群下与b2g对称性相关,在这种情况下,环面翻转选择规则为+/- <-- -/+。基态和第一激发扭转态的转动跃迁将被基态和激发振动态中的扭转分裂分开,实际上,我们观察到每个跃迁分裂为强度强和弱的成分,间隔约为0.0018 cm-1。再次使用刚性转子模型分别对强、弱跃迁集进行拟合,得到ν13(强) = 1240.34858(4) cm-1,B' = 0.0354192(7) cm-1,B'' = 0.0354355(7) cm-1以及ν13(弱) = 1240.34674(5) cm-1,B' = 0.0354188(9) cm-1,B'' = 0.0354360(7) cm-1。使用由邓宁及其同事开发的四重zeta质量的相关一致基组系列,在MP2和CCSD(T)理论水平上进行的高水平电子结构计算,对振动平均结构参数r(C-C) = 1.568 Å,r(C-F)α = 1.340 Å,r(C-F)β = 1.329 Å,α(F-C-F) = 110.3°,θz(C-C-C) = 89.1°,以及δ(C-C-C-C) = 14.°和转动常数A = B = 0.°354 cm-1和C = 0.°2898 cm-1给出了最佳估计,后者与实验测定值的偏差在0.00002 cm-1以内。使用MP2理论水平上的高能导数计算的非谐振动频率与实验测量的基频相差均在<27 cm-1(大多数情况下<5 cm-1)以内。我们在CCSD(T)/CBS(完备基组)极限下对环面翻转势垒的最佳估计为132 cm-1。对C4F8电子密度的分析表明,环面翻转势垒主要源于σCC→σCF超共轭相互作用,这种相互作用在环面形式中比平面形式中更能稳定分子结构。然而这种相互作用在C4F8中比在C4H8中稍弱,这一事实与前者(132 cm-1)相对于后者(498 cm-1)较小的势垒是一致的。