Miller Stephen R, Schultz Nathan E, Truhlar Donald G, Leopold Doreen G
Chemistry Department, University of Minnesota, 207 Pleasant Street S.E., Minneapolis, Minnesota 55455, USA.
J Chem Phys. 2009 Jan 14;130(2):024304. doi: 10.1063/1.3008056.
Computational results are reported for the ground and low-lying excited electronic states of Al(3)(-) and Al(3) and compared with the available spectroscopic data. In agreement with previous assignments, the six photodetachment transitions observed in the vibrationally resolved 488 nm photoelectron spectrum of Al(3)(-) are assigned as arising from the ground X (1)A(1) (')((1)A(1)) and excited (3)B(2) states of Al(3)(-) and accessing the ground X (2)A(1)(')((2)A(1)) and excited (2)A(2)(")((2)B(1)), (4)A(2), and (2)B(2) states of Al(3) (with C(2v) labels for D(3h) states in parentheses). Geometries and vibrational frequencies obtained by PBE0 hybrid density functional calculations using the 6-311+G(3d2f) basis set and energies calculated using coupled cluster theory with single and double excitations and a quasiperturbative treatment of connected triple excitations (CCSD(T)) with the aug-cc-pVxZ {x=D, T, Q} basis sets with exponential extrapolation to the complete basis set limit are in good agreement with experiment. Franck-Condon spectra calculated in the harmonic approximation, using either the Sharp-Rosenstock-Chen method which includes Duschinsky rotation or the parallel-mode Hutchisson method, also agree well with the observed spectra. Possible assignments for the higher-energy bands observed in the previously reported UV photoelectron spectra are suggested. Descriptions of the photodetachment transition between the Al(3)(-) and Al(3) ground states in terms of natural bond order (NBO) analyses and total electron density difference distributions are discussed. A reinterpretation of the vibrational structure in the resonant two-photon ionization spectrum of Al(3) is proposed, which supports its original assignment as arising from the X (2)A(1)(') ground state, giving an Al(3) bond dissociation energy, D(0)(Al(2)-Al), of 2.403+/-0.001 eV. With this reduction by 0.3 eV from the currently recommended value, the present calculated dissociation energies of Al(3), Al(3)(-), and Al(3)(+) are consistent with the experimental data.
报道了Al(3)(-)和Al(3)基态及低激发电子态的计算结果,并与现有的光谱数据进行了比较。与先前的归属一致,在Al(3)(-)的振动分辨488 nm光电子能谱中观察到的六个光解离跃迁被归属为源于Al(3)(-)的基态X (1)A(1) (')((1)A(1))和激发态(3)B(2),并跃迁到Al(3)的基态X (2)A(1)(')((2)A(1))和激发态(2)A(2)(")((2)B(1))、(4)A(2)和(2)B(2)(括号内为D(3h)态的C(2v)标记)。使用6 - 311+G(3d2f)基组通过PBE0杂化密度泛函计算得到的几何结构和振动频率,以及使用含单双激发的耦合簇理论和对连接三激发的准微扰处理(CCSD(T))并采用aug - cc - pVxZ {x = D, T, Q}基组并外推到完全基组极限计算得到的能量,与实验结果吻合良好。使用包含杜施金斯基转动的夏普 - 罗森斯托克 - 陈方法或平行模式哈钦森方法在谐振近似下计算的弗兰克 - 康登光谱,也与观测光谱吻合良好。对先前报道的紫外光电子能谱中观察到的高能带提出了可能的归属。讨论了基于自然键序(NBO)分析和总电子密度差分布对Al(3)(-)和Al(3)基态之间光解离跃迁的描述。提出了对Al(3)共振双光子电离光谱中振动结构的重新解释,支持其最初归属为源于X (2)A(1)(')基态,给出Al(3)的键解离能D(0)(Al(2)-Al)为2.403±0.001 eV。与当前推荐值相比降低了0.3 eV后,目前计算的Al(3)、Al(3)(-)和Al(3)(+)的解离能与实验数据一致。