首页> 外文期刊>The Journal of Chemical Physics >THE (3)A(2), (1)A(2), B-3(2), AND B-1(2) ELECTRONIC STATES OF CH2 - SMALL BOND ANGLE STATES
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THE (3)A(2), (1)A(2), B-3(2), AND B-1(2) ELECTRONIC STATES OF CH2 - SMALL BOND ANGLE STATES

机译:CH2的(3)A(2),(1)A(2),B-3(2)和B-1(2)电子态-小键角态

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Molecular structures with very small bond angles are a curiosity in chemistry. The two triplet ((3)A(2) and B-3(2)) and two singlet ((1)A(2) and B-1(2)) excited states of CH2 have been investigated systematically using ab initio electronic structure theory. For these four states total energies and physical properties including geometries, dipole moments, harmonic vibrational frequencies, and associated infrared intensities were determined with the single and double excitation configuration interaction (CISD) method using four different basis sets. It is confirmed in this study that the four states of CH2 all have bent structures with longer CH bond lengths and smaller bond angles than the four lower-lying ((X) over tilde, (a) over tilde (b) over tilde, and (c) over tilde) states of CH2. At the CISD optimized geometries single point energies were determined with complete active space self-consistent-held (CASSCF) and CASSCF second-order configuration interaction (SOCI) levels of theory. For the triplet excited states single point energies were also determined employing coupled cluster with single and double excitations (CCSD) and CCSD with perturbative triple excitations methods. At the CISD level with the largest basis set, the triple zeta plus triple polarizations with two sets of higher angular momentum and two sets of diffuse functions basis set [TZ3P(2f,2d) f2diff], the bond angles were predicted to be 40.6 degrees ((3)A(2)), 46.1 degrees ((1)A(2)), 76.3 degrees (B-3(2)), and 81.3 degrees (B-1(2)), while the dipole moments were determined to be 2.35 ((3)A(2)), 2.26 ((1)A(2)), 1.69 (B-3(2)), and 1.60 debye (B-1(2)), respectively. With the most accurate method in this study, the CASSCF-SOCI level with the TZ3P(2 f, 2d) + 2diff basis set, the energy separations (T-e value) between the ground state ((X) over tilde B-3(1)) and the four excited states were predicted to be 73.7 kcal/mol (3.20 eV, 25 800 cm(-1)) for the (3)A(2) state, 96.8 kcal/mol (4.20 eV, 33 800 cm(-1)) for the (1)A(2) state, 151.0 kcal/mol (6.55 eV, 52 800 cm(-1)) for the B-3(2) state, and 182.5 kcal/mol (7.91 eV; 63 800 cm(-1)) for the B-1(2) state, respectively. (C) 1997 American Institute of Physics. [References: 43]
机译:具有非常小的键角的分子结构是化学上的一个好奇心。 CH2的两个三重态((3)A(2)和B-3(2))和两个单重态((1)A(2)和B-1(2))的激发态已从头开始进行了系统研究结构理论。对于这四个状态,使用四个不同的基础集,通过单和双激发配置相互作用(CISD)方法确定了包括几何形状,偶极矩,谐波振动频率以及相关的红外强度在内的总能量和物理属性。在这项研究中已确认,CH2的四个状态均具有弯曲结构,与四个较低位置的(波浪线上方的(X),波浪线上方的(b)和波浪线上方的,以及(c)在波浪号上)。在CISD优化的几何结构中,通过理论上完整的活动空间自洽保持(CASSCF)和CASSCF二阶配置相互作用(SOCI)级别确定单点能量。对于三重激发态,还使用具有单激发和双激发的耦合簇(CCSD)和具有扰动三激发方法的CCSD确定了单点能量。在具有最大基础集,具有两组较高角动量和两组扩散函数基础集[TZ3P(2f,2d)f2diff]的三级zeta加三级极化的CISD级别上,键角预计为40.6度((3)A(2)),46.1度((1)A(2)),76.3度(B-3(2))和81.3度(B-1(2)),而偶极矩为分别确定为2.35((3)A(2)),2.26((1)A(2)),1.69(B-3(2))和1.60德拜(B-1(2))。使用本研究中最准确的方法,以TZ3P(2 f,2d)+ 2diff为基集的CASSCF-SOCI液位,在波浪线B-3(1)上的基态((X))之间的能量间隔(Te值) )),对于(3)A(2)状态,四个激发态预计为73.7 kcal / mol(3.20 eV,25 800 cm(-1)),96.8 kcal / mol(4.20 eV,33800 cm(-1)) (-1))(1)A(2)状态为151.0 kcal / mol(6.55 eV,52800 cm(-1))B-3(2)状态为182.5 kcal / mol(7.91 eV; B-1(2)状态分别为63 800 cm(-1))。 (C)1997美国物理研究所。 [参考:43]

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