首页> 外文期刊>The Journal of Chemical Physics >COUPLED-CLUSTER CALCULATIONS OF THE EXCITATION ENERGIES OF ETHYLENE, BUTADIENE, AND CYCLOPENTADIENE [Review]
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COUPLED-CLUSTER CALCULATIONS OF THE EXCITATION ENERGIES OF ETHYLENE, BUTADIENE, AND CYCLOPENTADIENE [Review]

机译:乙烯,丁二烯和环戊二烯激发能的耦合簇计算[综述]

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The equation-of-motion coupled-cluster (EOM-CC) method has been used to calculate the vertical excitation energies of ethylene, trans-butadiene, cis-butadiene, and cyclopentadiene. The approximations used were the EOM-CC singles-and-doubles (EOM-CCSD) method and EOM-CCSD with a noniterative treatment of triple excitations, EOM-CCSD(T), EOM-CCSD((T) over tilde). The basis sets were atomic natural orbital sets augmented with diffuse functions. Comparisons have been made with a series of complete active space second-order perturbation theory (CASPT2) results, which used the same basis sets and geometries, and experiment. For the Rydberg states the EOM-CCSD results were in good agreement with experiment and CASPT2. The results for the valence states show more variation. For ethylene CASPT2 exaggerates the Rydberg character of the V state, while EOM-CCSD provides a better description. For the valence states of the other molecules the EOM-CCSD excitation energies tend to be too high, but considerable improvements are given by EOM-CCSD((T) over tilde). For the 1(1)B(u)/1(1)B(2) states of butadiene and cyclopentadiene EOM-CCSD((T) over tilde) agrees well with experiment and CASPT2. The agreement for the 1(1)A(1)-->2(1)A(1) and 1(1)A(1)/2(1)A(1) transitions for tuans-butadiene and cis-butadiene, which are not known experimentally, is not so good, with the EOM-CC results significantly higher than the CASPT2 ones. However, the EOM-CCSD((T) over tilde) and CASPT2 energies for the 1(1)A(1)-->2(1)A(1) transition in cyclopentadiene are in quite close agreement and both agree well with experiment. EOM-CCSD(T) shows an average error in vertical excitation energies for all states of all molecules of 0.12 eV, and improves those for valence states from an error of 0.26 eV for EOM-CCSD to 0.13 eV. (C) 1996 American Institute of Physics. [References: 101]
机译:运动方程组(EOM-CC)方法已用于计算乙烯,反丁二烯,顺丁二烯和环戊二烯的垂直激发能。所使用的近似值是EOM-CC单打和双打(EOM-CCSD)方法和EOM-CCSD,并经过三重激励的非迭代处理,EOM-CCSD(T),EOM-CCSD((T代字号)。基本集是原子自然轨道集,具有扩散函数。使用一系列相同的基集和几何形状,并与一系列完整的活动空间二阶扰动理论(CASPT2)结果进行了比较。对于Rydberg,EOM-CCSD结果与实验和CASPT2吻合良好。价态的结果显示出更多的变化。对于乙烯,CASPT2夸大了V状态的Rydberg特性,而EOM-CCSD提供了更好的描述。对于其他分子的价态,EOM-CCSD的激发能往往太高,但EOM-CCSD((T)超过代字号)给出了相当大的改进。对于丁二烯和环戊二烯的1(1)B(u)/ 1(1)B(2)态,EOM-CCSD((T)代字号)与实验和CASPT2吻合良好。 ans丁二烯和顺丁二烯的1(1)A(1)-> 2(1)A(1)和1(1)A(1)/ 2(1)A(1)过渡的协议,这在实验上还不为人所知,效果不是很好,EOM-CC的结果明显高于CASPT2的结果。但是,环戊二烯中1(1)A(1)-> 2(1)A(1)跃迁的EOM-CCSD((T)高于代字号)和CASPT2能量非常接近,并且都与实验。 EOM-CCSD(T)显示所有分子的所有状态的垂直激发能的平均误差为0.12 eV,并将价态的误差从EOM-CCSD的误差为0.26 eV提高到0.13 eV。 (C)1996年美国物理研究所。 [参考:101]

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