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首页> 外文期刊>The Journal of Chemical Physics >Vacuum ultraviolet pulsed-field ionization-photoelectron study of H_2S in the energy range of 10-17 eV
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Vacuum ultraviolet pulsed-field ionization-photoelectron study of H_2S in the energy range of 10-17 eV

机译:能量范围为10-17 eV的H_2S真空紫外脉冲场电离-光电子研究

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摘要

Vacuum ultraviolet pulsed-field ionization-photoelectron(PFI-PE)spectra of H_2S have been recorded at PFI-PE resolutions of 0.6-1.0 meV in the energy range of 10-17 eV using high-resolution synchrotron radiation.The PFI-PE spectrum,which covers the formation of the valence electronic states H_2S~+(X~2B_1,A~2A_1,and B~2B_2),is compared to the recent high-resolution He I photoelectron spectra of H2S obtained by Baltzer et al [Chem.Phys.195,403(1995)].In addition to the overwhelmingly dominated origin vibrational band,the PFI-PE spectrum for H_2S~+(X~2B_1) is found to exhibit weak vibrational progressions due to excitation of the combination bands in the v_1~+ symmetric stretching and v_2~+ bending modes.While the ionization energy(IE)for H_2S~+(X~2B_1)obtained here is in accord with values determined in previously laser PFI-PE measurements,the observation of a new PFI-PE band at 12.642(+-)0.001 eV suggests that the IE for H_2S~+(A~2A_1)may be 0.12 eV lower than that reported in the He I study.The simulation of rotational structures resolved in PFI-PE bands shows that the formation of H_2S~+(X~2B_1)and H_2S~+(A~2A_1)from photoionization of H_2S(X ~1A_1) is dominated by type-C and type-5 transitions,respectively.This observation is consistent with predictions of the multichannel quantum defect theory.The small changes in rotational angular momentum observed are consistent with the dominant atomiclike character of the 2b_1 and 5a_1 molecular orbitals of H2S.The PFI-PE measurement has revealed perturbations of the(0,6,0)K~+=3 and (0,6,0)K~+=4 bands of H_2S~+(A~2A_1).Interpreting that these perturbations arise from Renner-Teller interactions at energies close to the common barriers to linearity of the H_2S~+(X~2B,and A ~2A,)states,we have deduced a barrier of 23 209 cm~(-1) for H_2S~+(X~2B_1)and 5668 cm~(-1) for H_2S~+(A ~2A_1).The barrier of 23 209 cm~(-1)for H_2S~+(X ~2B_1)is found to be in excellent agreement with the results of previous studies.The vibrational PFI-PE bands for H_2S~+(B ~2B_2)are broad,indicative of the predissociative nature of this state.
机译:使用高分辨率同步辐射在10-17 eV的能量范围内以0.6-1.0 meV的PFI-PE分辨率记录了H_2S的真空紫外脉冲场电离光电子光谱(PFI-PE)。将覆盖价电子态H_2S〜+(X〜2B_1,A〜2A_1和B〜2B_2)的形成与Baltzer等人最近获得的H2S高分辨率He I光电子能谱进行比较。 Phys.195,403(1995)]。除了绝大多数的原始振动带外,H_2S〜+(X〜2B_1)的PFI-PE谱还由于激发v_1〜中的组合带而表现出较弱的振动级数。 +对称拉伸和v_2〜+弯曲模式。虽然此处获得的H_2S〜+(X〜2B_1)的电离能(IE)与以前的激光PFI-PE测量中确定的值一致,但观察到了新的PFI-PE 12.642(+-)0.001 eV的谱带表明H_2S〜+(A〜2A_1)的IE可能比He I中报告的IE低0.12 eV在PFI-PE波段解析旋转结构的模拟表明,H_2S(X〜1A_1)的光电离形成H_2S〜+(X〜2B_1)和H_2S〜+(A〜2A_1)主要由C型决定。该观察与多通道量子缺陷理论的预测相符。观察到的旋转角动量的微小变化与H2S的2b_1和5a_1分子轨道的主要原子样特征相符。测量显示了H_2S〜+(A〜2A_1)的(0,6,0)K〜+ = 3和(0,6,0)K〜+ = 4个带的扰动。这些扰动是由Renner-在能量接近于H_2S〜+(X〜2B和A〜2A,)态的线性常见障碍的能量处的泰勒相互作用,我们推导出H_2S〜+(X〜)的势垒为23 209 cm〜(-1)。 H_2S〜+(A〜2A_1)为2B_1)和5668 cm〜(-1).H_2S〜+(X〜2B_1)为23209 cm〜(-1)的势垒与结果非常吻合PFI-PE振动b H_2S〜+(B〜2B_2)的和广泛,表明该状态的前离解性质。

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