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Cross sections for the two-step radiative decay process $$X(v)\rightarrow A(v^{\prime \prime })\rightarrow X(v^\prime )$$ X ( v ) → A ( v ″ ) → X ( v ′ ) in e -LiH collisions
The European Physical Journal D ( IF 1.5 ) Pub Date : 2021-05-20 , DOI: 10.1140/epjd/s10053-021-00164-x
Roberto Celiberto , Annarita Laricchiuta

Abstract

The cross sections for the two-step process, represented by the electron-impact vibro-electronic excitation \(X^1\varSigma ^+(v) \rightarrow A^1\varSigma ^+(v'')\) of the LiH molecule, followed by radiative decay back on the vibrational manifold of the ground state, \(A^1\varSigma ^+(v'')\rightarrow X^1\varSigma ^+(v')\), are calculated as a function of the incident electron energy from the threshold to 1000 eV. The final cross sections for the two-step process, which results in an overall vibrational excitation of the molecule, known also as E-v process, are provided for all the possible \(v,v'\) transitions among the vibrational levels, including the continuum, of the electronic ground state.

Graphic abstract



中文翻译:

两步辐射衰减过程的横截面$$ X(v)\ rightarrow A(v ^ {\ prime \ prime}} \ rightarrow X(v ^ \ prime)$$ X(v)→A(v'') →e -LiH碰撞中的X(v')

摘要

两步过程的横截面由电子冲击振动电子激发\(X ^ 1 \ varSigma ^ +(v)\ rightarrow A ^ 1 \ varSigma ^ +(v'')\表示LiH的分子,随后在基态的振动歧管辐射衰变背面,\(A ^ 1 \ varSigma ^ +(v '')\ RIGHTARROW X ^ 1 \ varSigma ^ +(v')\) ,被计算为从阈值到1000 eV的入射电子能量的函数。为两步过程的最终横截面提供了分子的整体振动激发(也称为Ev过程),用于所有振动水平之间可能的\(v,v'\)跃迁,包括跃迁。电子基态的连续体。

图形摘要

更新日期:2021-05-20
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