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Fragmentation of energy-selected SF5CF3+ probed by threshold photoelectron photoion coincidence spectroscopy: bond dissociation energy of SF5-CF3, and its atmospheric implications

机译:阈值光电子光合符合谱探测的能量选择SF5CF3 +的碎片化:SF5-CF3的键离解能及其大气意义

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摘要

Using tunable vacuum-UV radiation from a synchrotron in the range 12-26 eV, we have measured the threshold photoelectron and threshold photoelectron – photoion coincidence spectrum of SF\(_5\)CF\(_3\), a new anthropogenic greenhouse gas. The ground state of SF\(_5\)CF\(_3^+\) is repulsive in the Franck-Condon region, the parent ion is not observed, and the onset of ionisation can only give an upper limit to the energy of the first dissociative ionisation pathway of SF\(_5\)CF\(_3\), to CF\(_3^+\) + SF\(_5\) + e\(^-\). We have determined the kinetic energy released into the two fragments over a range of photon energies in the Franck-Condon region of the ground state of SF\(_5\)CF\(_3^+\). Using an impulsive model, the data has been extrapolated to zero kinetic energy to obtain a value for the first dissociative ionisation energy for SF\(_5\)CF\(_3\) of 12.9 \(\pm\) 0.4 eV. A similar experiment for CF\(_4\) to CF\(_3^+\) + F + e\(^-\)) and SF\(_6\) (to SF\(_5^+\) + F + e\(^-\)) yielded values for their dissociative ionisation energies of 14.45 \(\pm\) 0.20 and 13.6 \(\pm\) 0.1 eV, respectively, in agreement with previous data on the CF\(_3\) and SF\(_5\) free radicals. The enthalpy of formation at 0 K of SF\(_5\)CF\(_3\) is determined to be -1770 \(\pm\) 47 kJ mol\(^{-1}\), and the dissociation energy of the SF\(_5\)-CF\(_3\) bond at 0 K to be 392 \(\pm\) 48 kJ mol\(^{-1}\) or 4.06 \(\pm\) 0.45 eV. The implication of this bond strength is that SF\(_5\)CF\(_3\) is very unlikely to be broken down by UV radiation in the stratosphere. In addition, over the complete energy range of 12-26 eV, coincidence ion yields of SF\(_5\)CF\(_3\) have been determined. CF\(_3^+\) and SF\(_3^+\) are the most intense fragment ions, with SF\(_5^+\), SF\(_4^+\) and CF\(_2^+\) observed very weakly. Energetic constraints require that SF\(_3^+\), SF\(_4^+\) and CF\(_2^+\) can only form with CF\(_4\) + F, CF\(_4\) and SF\(_6\), respectively, so that fragmentation of SF\(_5\)CF\(_3^+\) to these ions involves migration of a fluorine atom across the S-C bond.
机译:利用同步加速器在12-26 eV范围内可调的真空-UV辐射,我们测量了新的人为温室气体SF \(_ 5 \)CF \(_ 3 \)的阈值光电子和阈值光电子-光子重合光谱。 SF \(_ 5 \)CF \(_ 3 ^ + \)的基态在弗兰克-康登区中是排斥性的,未观察到母离子,并且电离的开始只能给电子的能量提供一个上限。 SF \(_ 5 \)CF \(_ 3 \)到CF \(_ 3 ^ + \)+ SF \(_ 5 \)+ e \(^-\)的第一个解离电离途径。我们已经确定了SF \(_ 5 \)CF \(_ 3 ^ + \)基态的Franck-Condon区域内在一定范围的光子能量上释放到两个碎片中的动能。使用脉冲模型,已将数据外推至零动能,以获得SF \(_ 5 \)CF \(_ 3 \)的第一解离电离能值为12.9 \(\ pm \)0.4 eV。 CF \(_ 4 \)与CF \(_ 3 ^ + \)+ F + e \(^-\))和SF \(_ 6 \)(与SF \(_ 5 ^ + \)+ F + e \(^-\))的解离电离能值分别为14.45 \(\ pm \)0.20和13.6 \(\ pm \)0.1 eV,与CF \(_ 3 \)上的先前数据一致和SF \(_ 5 \)自由基。 SF \(_ 5 \)CF \(_ 3 \)在0 K时的形成焓被确定为-1770 \(\ pm \)47 kJ mol \(^ {-1} \),并且解离能为在0 K时的SF \(_ 5 \)-CF \(_ 3 \)键为392 \(\ pm \)48 kJ mol \(^ {-1} \)或4.06 \(\ pm \)0.45 eV。这种结合强度的暗示是SF \(_ 5 \)CF \(_ 3 \)不太可能被平流层中的紫外线辐射破坏。此外,在12-26 eV的整个能量范围内,已确定SF \(_ 5 \)CF \(_ 3 \)的重合离子产率。 CF \(_ 3 ^ + \)和SF \(_ 3 ^ + \)是最强的碎片离子,其中SF \(_ 5 ^ + \),SF \(_ 4 ^ + \)和CF \(_ 2 ^ + \ )观察非常微弱。能量约束要求SF \(_ 3 ^ + \),SF \(_ 4 ^ + \)和CF \(_ 2 ^ + \)只能与CF \(_ 4 \)+ F,CF \(_ 4 \)和分别为SF \(_ 6 \),因此SF \(_ 5 \)CF \(_ 3 ^ + \)碎裂成这些离子涉及到氟原子通过SC键的迁移。

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