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The electron affinities of PF and PF2

机译:PF和PF2的电子亲和力

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Theoretical investigations of the adiabatic electron affinities of PF and PF2 have been carried out. Large basis sets were used in this research, ranging from TZ2Pf+diff up to aug-cc-pVQZ. The theoretical methods applied here were Hartree-Fock self-consistent-held (SCF) theory, single and double excitation configuration interaction (CISD), single and double excitation coupled cluster (CCSD), and the CCSD(T) method, which adds perturbatively the connected triple excitations to the CCSD method. The results of this investigation show that three theoretical methods, DZP++ BHLYP, G2, and aug-cc-pVQZ CCSD(T) provide excellent agreement with each other for the adiabatic electron affinities of PF and PF2. The high level of theory used in this research suggests that the adiabatic electron affinity of PF is about 0.75 eV, and that of PF2 is about 0.76 eV. These predictions are in contrast to the experimental values of 3.4 eV (for PF) and 1.4-1.6 eV (for PF2). (C) 1998 American Institute of Physics. [S0021-9606(98)01703-6]. [References: 31]
机译:对PF和PF2的绝热电子亲和力进行了理论研究。在这项研究中使用了较大的基集,范围从TZ2Pf + diff到aug-cc-pVQZ。这里应用的理论方法是Hartree-Fock自洽保持(SCF)理论,单激励和双激励配置相互作用(CISD),单激励和双激励耦合簇(CCSD)和CCSD(T)方法,该方法扰动地增加了将三重激励连接到CCSD方法。这项研究的结果表明,三种理论方法DZP ++ BHLYP,G2和aug-cc-pVQZ CCSD(T)对于PF和PF2的绝热电子亲和力提供了极好的一致性。在这项研究中使用的高级理论表明,PF的绝热电子亲和力约为0.75 eV,PF2的绝热电子亲和力约为0.76 eV。这些预测与3.4 eV(对于PF)和1.4-1.6 eV(对于PF2)的实验值相反。 (C)1998美国物理研究所。 [S0021-9606(98)01703-6]。 [参考:31]

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