Setzer KD, Borkowska-Burnecka J, Zyrnicki W, Fink EH
Physikalische Chemie, Fachbereich 9, Bergische Universität-Gesamthochschule Wuppertal, Wuppertal, 42097, Germany
J Mol Spectrosc. 2000 Oct;203(2):244-248. doi: 10.1006/jmsp.2000.8179.
Emission spectra of two new electronic transitions of Pb(2) have been measured with a Fourier transform spectrometer in the 5200-8500 cm(-1) range. The emissions were observed from the afterglow of a microwave discharge in a mixture of Pb(x) vapor with hydrogen and argon carrier gas. By comparison with the results of ab initio calculations, the spectra are assigned to transitions from the lowest 1(g) and 1(u) states to the X(1)0(+)(g) ground state. The X(2)1(g) --> X(1)0(+)(g) transition between the fine-structure components of the X(3)Sigma(-)(g) ground state must be magnetic dipole in nature and thus is the first purely magnetic dipole fine-structure transition observed in the optical region. The 1(u) state is mostly a component of the low-lying inverted A(3)Pi(u) state and so is denoted A(2)1(u). Vibrational analyses have yielded the following electronic energies and vibrational constants for (208)Pb(2) (in cm(-1)): X(1)0(+)(g): omega(e) = 110.20(2), omega(e)x(e) = 0.341(2); X(2)1(g): T(e) = 5304.9(1), omega(e) = 120.57(7), omega(e)x(e) = 0.254(14); A(2)1(u): T(e) = 7817.5(2), omega(e) = 126.45(6), omega(e)x(e) = 0.399(11), where the numbers in parentheses are the standard deviations of the parameters. Copyright 2000 Academic Press.
利用傅里叶变换光谱仪在5200 - 8500厘米⁻¹范围内测量了Pb(2)两个新电子跃迁的发射光谱。这些发射是在Pb(x)蒸气与氢气和氩气载气的混合气体中微波放电的余辉中观察到的。通过与从头算结果比较,光谱被归属为从最低的1(g)和1(u)态到X(1)0(+)(g)基态的跃迁。X(3)Σ⁻(g)基态精细结构组分之间的X(2)1(g)→X(1)0(+)(g)跃迁本质上必定是磁偶极跃迁,因此是在光学区域观察到的首个纯磁偶极精细结构跃迁。1(u)态主要是低激发反转A(3)π(u)态的一个组分,所以记为A(2)1(u)。振动分析给出了(208)Pb(2)的下列电子能量和振动常数(单位为厘米⁻¹):X(1)0(+)(g):ω(e)=110.20(2),ω(e)x(e)=0.341(2);X(2)1(g):T(e)=5304.9(1),ω(e)=120.57(7),ω(e)x(e)=0.254(14);A(2)1(u):T(e)=7817.5(2),ω(e)=126.45(6),ω(e)x(e)=0.399(11),其中括号内的数字是参数的标准偏差。版权所有2000年,学术出版社。