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Computer modelling of a short-pulse excited dielectric barrier discharge xenon excimer lamp (lambda similar to 172 nm)

机译:短脉冲激发电介质阻挡放电氙准分子灯的计算机建模(λ类似于172 nm)

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A detailed rate-equation analysis has been used to simulate the plasma kinetics in a pulsed-excited dielectric barrier discharge in xenon, under operating conditions where the discharge structure is spatially homogeneous. The one-dimensional model, incorporating 14 species and 70 reaction processes, predicts results that are in good agreement with experimental measurements of the electrical characteristics, and optical (vaccum-ultraviolet (VUV) and visible) pulse shapes. The model reveals that electrical breakdown of the discharge gap occurs via a fast-moving ionization/excitation wavefront that starts close to the anode dielectric and propagates towards the cathode at similar to3 x 10(5) m s(-1). The wavefront appears as a result of successive avalanches of electrons that propagate across the discharge gap after release from the cathode dielectric. During breakdown, the mean electron energy in the bulk plasma is close to optimum for preferential excitation of the Xe* 1s(4,5) states that feed the VUV emitting Xe-2* excimer states. Calculations suggest that the overall conversion efficiency from electrical energy to VUV output in the plasma is greater than 60%, with >99% of the light output emitted in the VUV. Parasitic processes that act to reduce the key Xe* 1s(4,5) and Xe-2* populations are found to be essentially negligible. For pulsed excitation, the longer-term spatio-temporal behaviour of the electron/ions during the afterglow or inter-pulse period is important, resulting in a remnant 'pre-pulse' ion density of similar to10(15)m(-3) close to the cathode dielectric. These ions bombard the cathode during the subsequent excitation period to release the secondary (seed) electrons required to achieve electrical breakdown. [References: 59]
机译:在放电结构在空间上均质的工作条件下,详细的速率方程分析已用于模拟氙气中脉冲激发介电势垒放电中的等离子体动力学。一维模型包含14种物质和70个反应过程,预测的结果与电学特性以及光学(真空-紫外线(VUV)和可见)脉冲形状的实验测量结果非常吻合。该模型表明,放电间隙的电击穿是通过快速移动的电离/激发波阵面发生的,该波阵面开始靠近阳极电介质,并以接近3 x 10(5)m s(-1)的速度向阴极传播。波前的出现是由于从阴极电介质释放出来的电子连续雪崩横穿放电间隙传播的结果。在击穿过程中,体等离子体中的平均电子能量接近于Xe * 1s(4,5)态的优先激发,从而激发了发射Xe-2 *准分子的VUV。计算表明,等离子体中从电能到VUV输出的总转换效率大于60%,VUV发出的光输出的> 99%。发现可以减少关键Xe * 1s(4,5)和Xe-2 *种群的寄生过程基本可以忽略。对于脉冲激发,在余辉或脉冲间周期内电子/离子的长期时空行为很重要,从而导致剩余的“脉冲前”离子密度类似于10(15)m(-3)靠近阴极电介质。这些离子在随后的激发期间轰击阴极,以释放实现电击穿所需的二次电子(种子)。 [参考:59]

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