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Theoretical methods: LZ coupling=A08-m3ci1

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According to the atom-atom model for ion-pair formation in molecular collisions, chemi-ionization in two-body collisions takes place via pseudo-crossing of the potential energy surfaces of the interacting atoms [More on the model in a mesoscopic module (link type: 'IS ELABORATED IN/elucidated in/project/wider range'; target: MESO-m3c-mod]

Potential curves

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Fig. A08-m3ci1-F1 shows the lowest ionic and covalent potential curves of sodium iodide. The general shape of the curves is explained in a mesoscopic module[MESO-m3c-mod (link type: 'IS EXPLAINED IN/is detailed in/project/wider range'; target: MESO-m3c-mod#crossing curves], and the precise shape is determined in another module [The exact figure is generated in the Interpretation (link type: 'INPUT FROM'; target: Interpretation A08-m5bi]. The species of the ionic electronic state, indicating the symmetry and multiplicity properties, is given by $^1\MS^+$. By building up the molecule from the two separate neutral particles Na(2S1/2) and I(2P3/2), the LS-coupling gives rise to eight molecular states. One of them has the same species $^1\MS^+$ as the ionic state, which can according to the Neumann-Wigner rule give rise to transitions. We assume that we can ignore the exited covalent state, only taking into account the lowest states of the system, thus reducing the case to a two-state problem.
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Then, for our collision process, one of the eight collisions has the probability Pb for a diabatic transition at a single passage of the pseudo-crossing at Rc, given by the Landau-Zener formula [The formula is given in a mesoscopic module (link type: 'INPUT FROM/project/wider range'; target: MESO-m3c-mod#Pb)].

Summarising, the following approximations have been used:

1.
The Landau-Zener transition-probability formula.
2.
The use of the Landau-Zener formula to collisions where the distance of closest approach R0 and the distance of pseudo-crossing Rc are not well separated [Arguments against the applicability (link type: 'IS ARGUED IN/external'; target: R25)]
3.
The use of the diabatic potentials [These potentials are given in a mesoscopic module (link type: 'IS CLARIFIED IN/project/wider range'; target: MESO-m3c-mod#U(R)] in the classical deflection function in spite of small deformation of the curves at the pseudo-crossing.
4.
The use of a transition point in spite of a transition region around the pseudo-crossing predicted by the Landau-Zener theory.
5.
The neglect of rotational coupling so far [Compare this to the module about the rotation coupling (link type: 'IS COMPARED WITH/sq-next'; target: A08-m3ci2]