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作 者:章玉珠[1] 王广安[1] 沈中华[1] 倪晓武[1] 陆建[1]
出 处:《激光技术》2007年第6期659-662,共4页Laser Technology
基 金:国家自然科学基金资助项目(60578015)
摘 要:为了研究入射激光功率密度对等离子体冲击波力学效应的影响,利用波长1.06μm,脉冲能量42mJ^320mJ,脉宽10ns的Nd∶YAG激光作用在Al靶上,研究了冲量耦合系数Cm和激光功率密度I0的关系。实验发现靶材在离焦度χ不同时,Cm和I的变化关系相似,而对应的最佳功率密度明显不同。在功率密度由低慢慢升高过程中,冲量耦合系数先随功率密度升高而增加,升到最大值后随功率密度增加而减小。通过分析激光等离子体的吸收作用和离焦度不同时激光和靶相互作用机理的不同,认为Cm出现峰值主要是受等离子体屏蔽效应的影响,稀疏波的作用使得焦斑处最佳功率密度最大,而焦斑处空气击穿消耗能量导致焦后Cm峰值减小。The dependence of the mechanics effect to the target induced by laser on laser intensity was reported. The experiments were performed by focusing output pulses of the Nd:YAG laser( 10ns pulse width at 1.06μm wavelength and 42mJ 320mJ pulse energy) on aluminum targets mounted on a ballistic pendulum. The data showed that there were different optimum intensities which gave a maximum Cm, at different extant of depart from the focus(χ). And the impulse coupling coefficients (Cm) was determined hy similar functions of intensity in the different χ. The Cm increases slowly with the increasing of laser intensity and decreases after it gets maximum quantity. According to the absorption of the plasma and the different laser-target interaction mechanisms at the different x,the results show that there is the maximum Cm because of the plasma shielding effect;the optimum intensity is largest at the focus because of the effect caused by the rare faction wave and the maximum Cm atχ〉0 is smaller than the others due to the energy consuming of the air breakdown at the focus.
关 键 词:激光技术 功率密度 等离子体冲击波 冲量耦合系数
分 类 号:TN249[电子电信—物理电子学]
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