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Multipoint self-focusing of laser radiation in optical breakdown plasma

机译:光学击穿等离子体中激光辐射的多点自聚焦

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The interference structure of the laser light scattering cone behind the laser spark was observed for the first time. We propose consideration of the observed structure as a result of interference of the laser radiation, scattered by two or more self-focusing centers in laser spark air plasma. We have investigated the spatial distribution of the laser radiation scattered by the laser spark. These experiments differ from the previous ones by use of the four harmonics of Nd-laser radiation. As a source of radiation the Nd-laser installation was used with the master oscillator, operated on one transverse and longitudinal mode. The pulse duration was 10 ns, pulse energy - up to 20 J and beam divergence - 8 $DOT 10$+$MIN@5$/ rad. After the frequency conversion by means of the KDP crystals the second, third, and fourth harmonics radiation appeared with the energy up to 10 J (in fourth harmonic). In each of our experiments one laser harmonic radiation was focused into the hermetical chamber, filled with air (10 divided by 760 mm Hg). For the scattered radiation registration we photographed the scattering flat white screen, illuminated by this radiation. This screen was disposed parallel to the laser beam axis at the distance of 2 - 6 mm from it. We observed a cone-like symmetric respectively to the laser beam axis radiation scattering in the spark. That enables us to determine the maximum angle alpha of laser radiation deviation as a function of pressure p and wavelength lambda (or number of harmonic N). !3 (truncated)
机译:首次观察激光火花后面的激光散射锥的干涉结构。我们提出了由于激光辐射的干扰而认为观察到的结构,其在激光火花空等离子体中的两个或更多个自聚焦中心散射。我们研究了激光火花散射的激光辐射的空间分布。这些实验通过使用ND-Laser辐射的四个谐波不同于前一种。作为辐射源来源,ND激光装置与主振荡器一起使用,在一个横向和纵向模式下操作。脉冲持续时间为10 ns,脉冲能量 - 高达20 j和光束分配 - 8 $ dot 10 $ + $ min @ 5 $ / rad。在借助于KDP晶体的频率转换之后,第二,第三和第四次谐波辐射出现在高达10J的能量(第四次谐波)。在我们的每一个实验中,一个激光谐波辐射聚焦到密封室中,填充有空气(10除以760mm Hg)。对于散射的辐射登记,我们拍摄了由该辐射照射的散射平面白色屏幕。该屏幕与激光束轴平行地设置在距离它的距离2-6mm的距离。我们观察到分别于火花中的激光束轴辐射散射的锥形对称。这使我们能够确定激光辐射偏差的最大角度α,作为压力p和波长λ(或谐波n的数量)。 !3(截断)

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