首页> 外文期刊>The Journal of Chemical Physics >ABSORPTION SPECTRUM OF C-60 IN THE GAS PHASE - AUTOIONIZATION VIA CORE-EXCITED RYDBERG STATES
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ABSORPTION SPECTRUM OF C-60 IN THE GAS PHASE - AUTOIONIZATION VIA CORE-EXCITED RYDBERG STATES

机译:气态Ced态里德伯态中C-60在气相中的吸收光谱。

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The absolute absorption cross section of C-60 in the gas phase (830-870 K) was measured as a function of the photon energy (3.5-11.4 eV) (absorption spectrum). Absorption peaks at 7.87, 8.12, 8.29, 9.2 eV and a dip at 8.45 eV observed are assigned as Feshbach resonances in the photoexcitation involving superexcited states. The superexcited states responsible for the 7.87, 8.12, and 9.2 eV peaks are assigned to be core-excited Rydberg states converging to the second, the third and the fourth ionization limits of C-60 (8.89, 9.12, 10.82-11.59 eV), respectively. The 8.29 eV peak is considered to originate from vibrational excitation of a totally symmetric pentagonal pinch mode of the superexcited state responsible for the 8.12 eV peak. Further, a relative photoionization quantum yield was estimated from the absorption cross section measured and the relative photoionization cross section reported. The yield increases particularly in the vicinity of 8 eV in accordance with a high efficiency of autoionization of the superexcited states. Ionization efficiency is not high in the vicinity of the first ionization energy, probably because of rapid energy dissipation into its vibrational modes. The spectrum below the ionization energy resemble the absorption spectra of C-60 in its solutions. (C) 1996 American Institute of Physics. [References: 27]
机译:测量了C-60在气相(830-870 K)中的绝对吸收截面,其是光子能量(3.5-11.4 eV)(吸收光谱)的函数。在涉及超激发态的光激发中,在7.87、8.12、8.29、9.2 eV处的吸收峰和在8.45 eV处的下降被指定为Feshbach共振。负责7.87、8.12和9.2 eV峰的超激发态被指定为核心激发的里德堡态,收敛到C-60的第二,第三和第四电离极限(8.89、9.12、10.82-11.59 eV),分别。 8.29 eV峰被认为是由负责8.12 eV峰的超激发态的完全对称五边形收缩模式的振动激发引起的。此外,从测量的吸收截面估计相对光电离量子产率,并报告相对光电离截面。根据超激发态的高电离效率,特别是在8 eV附近,产率增加。在第一电离能附近,电离效率不高,可能是由于快速将能量耗散到其振动模式中。低于电离能的光谱类似于C-60在其溶液中的吸收光谱。 (C)1996年美国物理研究所。 [参考:27]

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