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首页> 外文期刊>The Journal of Chemical Physics >STATE-TO-STATE RATE CONSTANTS FOR THE COLLISIONAL INTERACTION OF XE(7P), XE(6P'), AND KR(5P') ATOMS WITH HE AND AR
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STATE-TO-STATE RATE CONSTANTS FOR THE COLLISIONAL INTERACTION OF XE(7P), XE(6P'), AND KR(5P') ATOMS WITH HE AND AR

机译:XE(7P),XE(6P')和KR(5P')原子与HE和AR碰撞相互作用的状态间速率常数

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One-photon laser excitation of Xe(6s[3/2](2)) and Kr(5s[3/2](2)) atoms that were generated in a discharge-flow reactor was used to study the collisional relaxation of the Kr(5p'[3/2](1), [3/2](2), and [1/2](1)), the Xe(7p[3/2](2), [3/2](1), [5/2](2), and [5/2](3)), and the Xe(6p'[3/2](1), [3/2](2), and [1/2](1)) states in He and Ar. Both cw and pulsed laser excitation techniques were utilized to obtain the total deactivation rate constants and product formation rate constants at 300 K. Collisions with He mainly produce Xe* and Kr* product states with small energy defects, but the rate constants can be as large as 20X10(-10) cm(3) atom(-1) s(-1) which correspond to thermally averaged cross sections of 150 Angstrom(2). Because of the rapid collisional coupling of populations in nearly isoenergetic levels, multicomponent exponential decay of the initially produced state is frequently observed. The deactivation rate constants for Ar are smaller than for He, but the product distributions tend to be more diverse than for He, and arguments based only on energy defects are riot necessarily a good guide to the favored product state(s) from Ar collisions. The magnitude of the quenching cross sections for Ar is consistent with the crossing of an entrance channel with several diabatic exit channel potentials. However, the superlarge quenching cross sections for Xe*-He to just one or two product levels require special considerations. The Kr(5p') and Xe(6p' and 7p) rate constants with He are discussed with respect to collisional effects upon the use of cw optical pumping to convert populations in the metastable Xe(6s[3/2](2)) and Kr(5s[3/2](2)) levels to the Xe(6s'[1/2](0)) and Kr(5s'[1/2](0)) levels. (C) 1996 American Institute of Physics. [References: 53]
机译:利用放电流反应器中产生的Xe(6s [3/2](2))和Kr(5s [3/2](2))原子的单光子激光激发研究了碳纳米管的碰撞弛豫Kr(5p'[3/2](1),[3/2](2)和[1/2](1)),Xe(7p [3/2](2),[3/2 ](1),[5/2](2)和[5/2](3))以及Xe(6p'[3/2](1),[3/2](2)和He和Ar中的[1/2](1))状态。连续激光和脉冲激光激发技术都用于获得300 K时的总失活速率常数和产物形成速率常数。与He的碰撞主要产生具有较小能量缺陷的Xe *和Kr *产物态,但速率常数可以大作为20X10(-10)cm(3)原子(-1)s(-1)对应于150埃(2)的热平均截面。由于群体在几乎等能量的水平上快速碰撞耦合,因此经常观察到初始产生状态的多组分指数衰减。 Ar的失活速率常数小于He的失活速率常数,但是产物的分布往往比He的多,并且仅基于能量缺陷的论点必然成为从Ar碰撞中偏爱的产物状态的良好指南。 Ar的淬火横截面的大小与具有几个非绝热出口沟道电势的入口沟道的交叉一致。但是,Xe * -He的超大淬火截面只有一两个产品级别需要特别考虑。关于He的Kr(5p')和Xe(6p'和7p)速率常数,讨论了使用cw光学泵浦转换亚稳Xe(6s [3/2](2))中的种群时的碰撞效应。和Kr(5s [3/2](2))电平分别达到Xe(6s'1 / 2(0))和Kr(5s'1 / 2(0))电平。 (C)1996年美国物理研究所。 [参考:53]

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