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Laser ablation of metals and semiconductors with 100 ps to 100 μs pulses

机译:以100 ps至100μs的脉冲对金属和半导体进行激光烧蚀

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摘要

Laser ablation of aluminum, silicon, titanium, germanium, and indium antimonide at 1064 nm in ambient laboratory air with pulse durations ranging from 100 ps to 100 μs has been characterized with optical microscopy. Highly focused spots of 10 μm yields fluences of 0.004 to 25 kJ/cm~2 and irradiances spanning 4 × 106-10~(14) W/cm~2. Single pulse hole depths range from 84 nm to 147 μm. A one-dimensional thermal model establishes a set of nondimensional variables for hole depth, fluence, and pulse duration. For pulse durations shorter than the radial diffusion time, the hole depth exceeds the thermal diffusion length by a factor of 1 to 30 for more than 90% of the data. For pulses longer than this critical time, transverse heat conduction losses dominate and holes as small as 10~(-3) times the thermal diffusion depth are produced. For all cases, the ablation efficiency, defined as atoms removed per incident photon, is 10(-2) or less, and is inversely proportional to volume removed for pulse durations less than 100 ns. At high fluences, more than 10 to 100 times ablation threshold, explosive boiling is identified as the likely mass removal mechanism, and hole depth scales approximately as fluence to 0.3 to 0.4 power. The power-law exponent is inversely proportional to the shielding of the laser pulse by ejected material, and shielding is maximum at the 1-ns pulse duration and minimum near the 1-μs pulse duration for each material. Using the thermal scaling variables, the high-fluence behavior for each material becomes strikingly similar.
机译:光学显微镜已经表征了在实验室环境空气中在1064 nm处对铝,硅,钛,锗和锑化铟的激光烧蚀,脉冲持续时间为100 ps至100μs。高聚焦点10μm产生的通量为0.004至25 kJ / cm〜2,辐照度为4×106-10〜(14)W / cm〜2。单脉冲孔深度范围为84 nm至147μm。一维热模型为孔深,通量和脉冲持续时间建立了一组无量纲变量。对于比径向扩散时间短的脉冲持续时间,对于超过90%的数据,孔深度比热扩散长度超出1到30倍。对于比该临界时间长的脉冲,横向导热损失占主导地位,并且产生的孔洞是热扩散深度的10〜(-3)倍。对于所有情况,烧蚀效率定义为每个入射光子去除的原子,等于或小于10(-2),并且与脉冲持续时间小于100 ns去除的体积成反比。在高通量下,大于10到100倍的消融阈值,爆炸沸腾被认为是可能的质量去除机制,孔深度范围大约是0.3到0.4功率的通量。幂律指数与喷射材料对激光脉冲的屏蔽成反比,对于每种材料,屏蔽在1 ns脉冲持续时间内最大,在1μs脉冲持续时间附近最小。使用热定标变量,每种材料的高通量行为都变得极为相似。

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