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首页> 外文期刊>Russian journal of physical chemistry, B. >Electron-Vibrational Energy Exchange in Collisions of Ar Atomsin the 3P2 Metastable State with N_2(X~lΣ_g~+)Molecules
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Electron-Vibrational Energy Exchange in Collisions of Ar Atomsin the 3P2 Metastable State with N_2(X~lΣ_g~+)Molecules

机译:N_2(X〜lΣ_g〜+)分子在3P2亚稳态的Ar原子碰撞中的电子振动能量交换

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摘要

Rate constants for electron-vibrational energy exchange Ar(3P,) + N_2,(X~1Σ_g~+, v = 0) →Ar(IS0) + N_2(C~Π_u, v'), wherev =0, 1, 2, were calculated. Calculations were performed taking into account the presence of a resonance in electron scattering by N2(X~1Σ_g~+). As a result, the interaction of Ar(3P,) withN~2(X~1Σ_g~+,v= 0) was characterized by attraction and, in the end, intersection of electron-vibrational potential surfaces correlating with Ar(3P2) + N_2(X~1Σ_g~+,v=0) and Ar('S0) + N,(C~3Π_u,at interparticle distances of2.5-3.5 A. Exchange interaction at which electron-vibrational transitions in the region of intersection ofelectron-vibrational potential surfaces accompanied by spin exchange were induced was calculated by theasymptotic method. The rate constants determined at 300-600 K were on the order of 10-11—and weakly increased as the temperature grew Mainly the C3Π_u, v = 0 state of the N, molecule was popu-lated. The calculation results were in satisfactory agreement with the experimental data obtained at 300 K.
机译:电子振动能量交换的速率常数Ar(3P,)+ N_2,(X〜1Σ_g〜+,v = 0)→Ar(IS0)+ N_2(C〜Π_u,v'),其中v = 0,1,2 ,进行了计算。考虑到N2(X〜1Σ_g〜+)在电子散射中存在共振,进行了计算。结果,Ar(3P,)与N〜2(X〜1Σ_g〜+,v = 0)的相互作用以吸引为特征,最后,与Ar(3P2)+相关的电子振动势能面相交N_2(X〜1Σ_g〜+,v = 0)和Ar('S0)+ N,(C〜3Π_u,在2.5-3.5 A的粒子间距离。交换相互作用,在此相互作用下电子在电子交界处发生振动转变通过渐近法计算出了伴随自旋交换的-振动势能面,在300-600 K下确定的速率常数约为10-11,并随温度的升高而微弱增加。主要是C3Π_u,v = 0计算结果与300 K下的实验数据吻合良好。

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