首页> 外文期刊>The Journal of Chemical Physics >High-resolution pulses field ionization photoelectron study of O-2: Predissociation lifetimes and high-n Rydberg lifetimes converging to O-2(+)(c (4)Sigma(-)(u), v(+)=0,1)
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High-resolution pulses field ionization photoelectron study of O-2: Predissociation lifetimes and high-n Rydberg lifetimes converging to O-2(+)(c (4)Sigma(-)(u), v(+)=0,1)

机译:O-2的高分辨率脉冲场电离光电子研究:离解寿命和高n Rydberg寿命收敛到O-2(+)(c(4)Sigma(-)(u),v(+)= 0,1 )

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摘要

We have measured the pulsed field ionization photoelectron (PFI-PE) spectrum of O-2 in the energy range of 24.53-25.0 eV at a PFI-PE resolution of 11 cm(-1) (full Width at half maximum, FWHM), The PFI-PE bands for O-2(+)(c (4)Sigma(u)(-), nu(+) = 0 and 1) obtained at O-2 rotational temperatures of 35 and 298 K have been simulated using the Buckingham-Orr-Sichel. model. Only the Delta N = -3, -1, +1, and +3 (or N, P, R, and T) rotational branches are observed, indicating that the outgoing electron continuum channels with angular momenta l=0, 2, and 4 dominate in-the threshold ionization transitions O-2(+)(c (4)Sigma(u)(-), nu(+) = 0 to 1, N+)<-- O-2(X (3)Sigma(g)(-), nu "=0, N "). The simulation yields natural rotational linewidths of 19.6+/-2.0 and 77+/-8 cm(-1) (FWHM) for the respective nu(+) = 0 and 1 PFI-PE bands of the O-2(+)(c (4)Sigma(u)(-)) state. These linewidths make possible the determination of the predissociation lifetimes for the nu(+) = 0 and 1 levels of O-2(+)(c (4)Sigma(u)(-)) to be (2.7+/-0.3) X 10(-13) and (6.9+/-0.7) X 10(-14) s, respectively. This experiment also provides accurate ionization energies of 24.5622(7)+/-0.0005 and 24.7544(5)+/-0.0005 eV for transitions to O-2(+)(c (4)Sigma(u)(-), nu(+)=0, N+=0) and O-2(+)(c (4)Sigma(u)(-), nu(+)=1, N+=0); from O-2(X (3)Sigma(g)(-), nu ", N "=1), respectively. The rotational constants of 1.58+/-0.02 and 1.54+/-0.04 cm(-1) obtained here for the O-2(+)(c (4)Sigma(u)(-) nu(+)=0) and O-2(+)(c (4)Sigma(u)(-), nu(+)=1) states allow the calculation of their corresponding equilibrium bond distances to be 1.155+/-0.011 and 1.170+/-0.015 Angstrom. The (nominal) effective lifetimes for,high-n Rydberg states converging to the O-2(+)(c (4)Sigma(u)(-), nu(+)=0 and 1) states are measured to be approximate to 0.33 mu S, which are significantly shorter than the values of approximate to 1.9 mu s measured for the O-2(+)(b (4)Sigma(g)(-), nu(+)=0-5) states. The shorter (nominal) effective lifetimes for high-n Rydberg states converging to O-2(+)(c (4)Sigma(g)(-), nu(+)=0 and 1) observed are attributed to the higher kinetic energy releases (or velocities) of O+ fragments resulting from predissociation;of the O-2(+) ion cores. (C) 1998 American Institute of Physics. [References: 35]
机译:我们测量了O-2的脉冲场电离光电子(PFI-PE)光谱,其能量范围为24.53-25.0 eV,PFI-PE分辨率为11 cm(-1)(半高全宽,FWHM),在O-2旋转温度为35和298 K下获得的O-2(+)(c(4)Sigma(u)(-),nu(+)= 0和1)的PFI-PE带已使用白金汉-奥尔-西歇尔。模型。仅观察到Delta N = -3,-1,+ 1和+3(或N,P,R和T)旋转分支,这表明出射电子连续谱通道的角动量为l = 0、2和。 4个主要阈值电离跃迁O-2(+)(c(4)Sigma(u)(-),nu(+)= 0至1,N +)<-O-2(X(3)Sigma (g)(-),nu“ = 0,N”)。对于相应的nu(+)= 0和O-2(+)(1)的1个PFI-PE谱带,模拟产生的自然旋转线宽为19.6 +/- 2.0和77 +/- 8 cm(-1)(FWHM) c(4)Sigma(u)(-))状态。这些线宽可以确定nu(+)= 0和1级O-2(+)(c(4)Sigma(u)(-))的解离寿命为(2.7 +/- 0.3) X 10(-13)和(6.9 +/- 0.7)X 10(-14)s。该实验还提供了准确的电离能24.5622(7)+/- 0.0005和24.7544(5)+/- 0.0005 eV,可转换为O-2(+)(c(4)Sigma(u)(-),nu( +)= 0,N + = 0)和O-2(+)(c(4)Sigma(u)(-),nu(+)= 1,N + = 0);分别来自O-2(X(3)Sigma(g)(-),nu“,N” = 1)。对于O-2(+)(c(4)Sigma(u)(-)nu(+)= 0)和此处获得的旋转常数1.58 +/- 0.02和1.54 +/- 0.04 cm(-1)和O-2(+)(c(4)Sigma(u)(-),nu(+)= 1)状态允许计算其对应的平衡键距离为1.155 +/- 0.011和1.170 +/- 0.015埃。高N里德堡态收敛至O-2(+)(c(4)Sigma(u)(-),nu(+)= 0和1)态的(标称)有效寿命被测量为近似值到0.33μS,这比O-2(+)(b(4)Sigma(g)(-),nu(+)= 0-5)状态下测得的大约1.9μs的值短得多。高n里德堡态收敛到O-2(+)(c(4)Sigma(g)(-),nu(+)= 0和1)的较短(标称)有效寿命是由于较高的动力学由于O-2(+)离子核的预离解而产生的O +碎片的能量释放(或速度)。 (C)1998美国物理研究所。 [参考:35]

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