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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Radiation trapping of the P-3(1)-S-1(0) resonant transitions of xenon and krypton in Xe-Kr, Xe-Ar, and Kr-Ar mixtures: Kinetic analysis and determination of the van der Waals broadening coefficients - art. no. 052721
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Radiation trapping of the P-3(1)-S-1(0) resonant transitions of xenon and krypton in Xe-Kr, Xe-Ar, and Kr-Ar mixtures: Kinetic analysis and determination of the van der Waals broadening coefficients - art. no. 052721

机译:Xe-Kr,Xe-Ar和Kr-Ar混合物中氙和rypto的P-3(1)-S-1(0)共振跃迁的辐射俘获:动力学分析和范德华扩展系数的测定-艺术。没有。 052721

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This work concerns radiation trapping of the 123-nm krypton and 147-nm xenon lines, in the presence of a lighter rare gas, as well as the study of the decay processes of the relevant resonant states due to inelastic collisions. It deals with Kr-Ar, Xe-Kr, and Xe-Ar mixtures. Pulsed, brief selective excitation of the Xe(P-3(1)) or Kr(P-3(1)) resonant states by three-photon absorption was achieved by means of a tunable dye laser. Spectral and temporal analysis was then performed. The time resolved luminescence, filtered in the vacuum ultraviolet region, obeys a decay law described by the sum of two exponential terms which are attributed to the deexcitation of the P-3(1) and P-3(2) states. The decay constants are estimated by the maximum likelihood method applied to a Poisson statistical law. In order to correctly determine the collision rate constants, it is important to account for variations of the apparent lifetime according to the gas concentration. Analysis of both systematic experimental errors and statistical errors leads to a good estimation of the accuracy of the results obtained. For each mixture, the variation of the time constants as a function of partial pressures allows a determination of the resonance broadening coefficient and van der Waals broadening coefficient of the transition studied, as well as the two- and three-body inelastic collision rates relative to the P-3(1) and P-3(2) states. There exists no energy transfer between the two gases. For binary rare-gas mixtures, where only the heavier gas is excited, homonuclear and heteronuclear three-body reactions account for the decay of the P-3(1) state. Nevertheless, for the P-3(2) State we observe both two- and three-body collisions. In order to simulate resonance radiation trapping, a numerical method based upon Monte Carlo techniques was used. Calculations were first performed and validated for an infinite cylinder. The difference between calculation and experiment was less than 1%. Then the program was adapted to our real experimental conditions and applied to the binary mixtures studied. A good agreement was found between experiments and calculations. Furthermore, our program allows us to obtain information not easily obtained experimentally. [References: 99]
机译:这项工作涉及在较轻的稀有气体存在下捕获123 nm rypto和147 nm氙线的辐射,以及研究由于非弹性碰撞而引起的相关共振态的衰减过程。它处理Kr-Ar,Xe-Kr和Xe-Ar混合物。 Xe(P-3(1))或Kr(P-3(1))共振态的脉冲,短暂的选择性激发通过三光子吸收是通过可调染料激光器实现的。然后进行光谱和时间分析。在真空紫外线区域中过滤的时间分辨发光遵循由两个指数项之和所描述的衰减定律,这两个衰减项归因于P-3(1)和P-3(2)状态的去激发。衰减常数通过应用于泊松统计定律的最大似然法估算。为了正确地确定碰撞速率常数,重要的是要考虑表观寿命根据气体浓度的变化。对系统实验误差和统计误差的分析都可以很好地估计获得的结果的准确性。对于每种混合物,时间常数作为分压的函数的变化可以确定所研究的跃迁的共振展宽系数和范德华展宽系数,以及相对于两体和三体的非弹性碰撞速率P-3(1)和P-3(2)状态。两种气体之间不存在能量转移。对于只有稀有气体被激发的二元稀有气体混合物,同核和异核三体反应可解释P-3(1)状态的衰减。但是,对于P-3(2)状态,我们同时观察到了两个和三个物体的碰撞。为了模拟共振辐射捕获,使用了基于蒙特卡洛技术的数值方法。首先进行计算并验证无限圆柱体。计算与实验之间的差异小于1%。然后将该程序调整为适合我们的实际实验条件,并应用于所研究的二元混合物。实验和计算之间找到了很好的协议。此外,我们的程序允许我们获得不容易通过实验获得的信息。 [参考:99]

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