首页> 外文期刊>IEEE journal of selected topics in quantum electronics >Plasma formation in water by picosecond and nanosecond Nd:YAG laser pulses. I. Optical breakdown at threshold and superthreshold irradiance
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Plasma formation in water by picosecond and nanosecond Nd:YAG laser pulses. I. Optical breakdown at threshold and superthreshold irradiance

机译:皮秒和纳秒Nd:YAG激光脉冲在水中形成等离子体。 I.阈值和超阈值辐照度下的光击穿

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We investigated plasma formation in distilled water by 30-ps and 6-ns Nd:YAG laser pulses of 1064-nm and 532-nm wavelength for focusing angles between 1.7/spl deg/ and 32/spl deg/. We determined the optical breakdown thresholds and analyzed the plasma length achieved at superthreshold irradiance, The parameter range investigated covers the parameters used for intraocular laser surgery. The experimental results are compared to theoretical models for the calculation of breakdown thresholds and the description of plasma growth for superthreshold breakdown. We found that at /spl lambda/=1064 nm the measured thresholds for both pulse durations coincide with the calculated thresholds for the generation of seed electrons by multiphoton ionization. The breakdown process is completed by avalanche ionization. The seed electron density required for breakdown is about 4/spl times/10/sup 9/ cm for the 6-ns pulses, and 1.4/spl times/10/sup 11/ cm/sup -3/ for the 30-ps pulses. No spot size dependence of the irradiance threshold for breakdown was observed. The average threshold is by a factor of 5.9 higher for 30-ps pulses (I/sub th/=4.5/spl times/1011 W/cm/sup 2/) than for 6-ns pulses (I/sub th/=0.76/spl times/10/sup 11/ W/cm/sup 2/). At angles below approximately 2/spl deg/, the threshold is influenced by self-focusing effects. The breakdown thresholds at 532 nm are slightly lower than at 1064 nm. Here, multiphoton ionization contributes considerably to the generation of free electrons throughout the whole process of plasma formation. Our results for plasma formation at superthreshold energies support a "breakdown wave" mechanism of plasma growth. For picosecond pulses, the breakdown threshold can be considered to be time-invariant, but for nanosecond pulses there is probably a decrease of the threshold during the laser pulse which may be due to UV-radiation emitted from plasma created at the beginning of the pulse.
机译:我们研究了蒸馏水中的等离子体形成情况,这些波长为10ps波长和1064nm和532nm波长的30-ps和6ns的Nd:YAG激光脉冲,聚焦角在1.7 / spl deg /和32 / spl deg /之间。我们确定了光学击穿阈值,并分析了在超阈值辐照下获得的等离子体长度。研究的参数范围涵盖了用于眼内激光手术的参数。将实验结果与理论模型进行比较,以计算击穿阈值并描述超阈值击穿的等离子体生长。我们发现在/ spl lambda / = 1064 nm处,两个脉冲持续时间的测量阈值与通过多光子电离产生种子电子的计算阈值一致。击穿过程通过雪崩电离完成。击穿所需的种子电子密度对于6 ns脉冲约为4 / spl次/ 10 / sup 9 / cm,对于30 ps脉冲约为1.4 / spl次/ 10 / sup 11 / cm / sup -3 / 。没有观察到击穿的辐照阈值的光斑尺寸依赖性。 30 ps脉冲(I / sub th / = 4.5 / spl乘以1011 W / cm / sup 2 /)的平均阈值比6 ns脉冲(I / sub th / = 0.76)高5.9倍/ spl times / 10 / sup 11 / W / cm / sup 2 /)。在小于大约2 / spl deg /的角度下,阈值受自聚焦效应的影响。 532 nm处的击穿阈值略低于1064 nm处的击穿阈值。在此,多光子电离在等离子体形成的整个过程中极大地促进了自由电子的产生。我们在超阈值能量下形成等离子体的结果支持了等离子体生长的“击穿波”机制。对于皮秒脉冲,击穿阈值可以认为是时不变的,但是对于纳秒脉冲,在激光脉冲过程中阈值可能会降低,这可能是由于脉冲开始时产生的等离子体发出的紫外线辐射引起的。 。

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