Boulanger Anne-Marie, Rennie Emma E, Holland David M P, Shaw David A, Mayer Paul M
Chemistry Department, University of Ottawa, Ottawa, Ontario K1N 6N5, Canada.
J Phys Chem A. 2006 Jul 13;110(27):8563-71. doi: 10.1021/jp0555854.
The valence shell electronic structures of methylhydrazine (CH(3)NHNH(2)), 1,1-dimethylhydrazine ((CH(3))(2)NNH(2)) and tetramethylhydrazine ((CH(3))(4)N(2)) have been studied by recording threshold and conventional (kinetic energy resolved) photoelectron spectra. Ab initio calculations have been performed on ammonia and the three methyl substituted hydrazines, with the structures being optimized at the B3-LYP/6-31+G(d) level of theory. The ionization energies of the valence molecular orbitals were calculated using the Green's function method, allowing the photoelectron bands to be assigned to specific molecular orbitals. The ground-state adiabatic and vertical ionization energies, as determined from the threshold photoelectron spectra, were IE(a) = 8.02 +/- 0.16 eV and IE(v) = 9.36 +/- 0.02 eV for methylhydrazine, IE(a) = 7.78 +/- 0.16 eV and IE(v) = 8.86 +/- 0.01 eV for 1,1-dimethylhydrazine and IE(a) = 7.26 +/- 0.16 eV and IE(v) = 8.38 +/- 0.01 eV for tetramethylhydrazine. Due to the large geometry change that occurs upon ionization, these IE(a) values are all higher than the true thresholds. New features have been observed in the inner valence region and these have been compared with similar structure in the spectrum of hydrazine. The effect of resonant autoionization on the threshold photoelectron yield is discussed. New heats of formation (Delta(f)H) are proposed for the three hydrazines on the basis of G3 calculations: 107, 94, and 95 kJ/mol for methylhydrazine, 1,1-dimethyhydrazine and tetramethylhydrazine, respectively. The previously reported Delta(f)H for tetramethylhydrazine is shown to be erroneous.
通过记录阈值光电子能谱和常规(动能分辨)光电子能谱,研究了甲基肼(CH(3)NHNH(2))、1,1 - 二甲基肼((CH(3))(2)NNH(2))和四甲基肼((CH(3))(4)N(2))的价层电子结构。对氨以及三种甲基取代肼进行了从头算计算,结构在B3 - LYP/6 - 31 + G(d)理论水平上进行了优化。使用格林函数方法计算了价分子轨道的电离能,从而能够将光电子能带归属到特定的分子轨道。由阈值光电子能谱确定的基态绝热电离能和垂直电离能,对于甲基肼,IE(a) = 8.02 ± 0.16 eV,IE(v) = 9.36 ± 0.02 eV;对于1,1 - 二甲基肼,IE(a) = 7.78 ± 0.16 eV,IE(v) = 8.86 ± 0.01 eV;对于四甲基肼,IE(a) = 7.26 ± 0.16 eV,IE(v) = 8.38 ± 0.01 eV。由于电离时发生较大的几何结构变化,这些IE(a)值均高于真实阈值。在内层价区观察到了新特征,并与肼光谱中的类似结构进行了比较。讨论了共振自电离对阈值光电子产率的影响。基于G3计算,提出了三种肼的新生成热(Δ(f)H):甲基肼为107 kJ/mol,1,1 - 二甲基肼为94 kJ/mol,四甲基肼为95 kJ/mol。结果表明之前报道的四甲基肼的Δ(f)H是错误的。