高功率飞秒激光在空气中传播时形成的高强度光通道

D. V. Apeksimov, Y. Geints, A. Zemlyanov, A. Iglakova, G. Matvienko, O. Minina, V. Oshlakov, A. V. Petrov
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引用次数: 0

摘要

本文从实验和理论两方面研究了高功率飞秒激光在空气中以成丝模式传播的小尺度横向结构的演化。利用钛蓝宝石激光器飞秒脉冲的宽孔径(厘米)准直光束获得了实验结果。结果确定了直径为几毫米的空间隔离高强光通道的传播特性。它们的形成是由于激光束初始横截面强度不均匀性的克尔自聚焦。结果表明,灯丝的形成(一种局部光结构,其存在与等离子体的形成和锥形发射的产生有关)并不发生在每个通道中。对该光通道特性进行了理论评价。它是基于飞秒激光脉冲单灯丝的衍射射线模型。对半径为厘米、功率为亚太瓦的激光束沿空气路径的横向演化曲线进行了研究,结果表明,产生激光丝化的强度不均匀的初始半径为几(2.5 ~ 3.5)毫米。这些不均匀性中的功率从19到26吉瓦不等。这些非均匀性的半径值和功率值的不同是它们发生自聚焦的距离与激光脉冲源不同的原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
High-intensity light channels formed during the propagation of high-power femtosecond laser radiation in air
The evolution of the small-scale transverse structure of high-power femtosecond laser radiation propagating in air in the filamentation mode has been experimentally and theoretically studied. Experimental results were obtained using wideaperture (centimeter) collimated beams of femtosecond pulses of a titanium-sapphire laser. As a result, the features of propagation of spatially isolated high-intensity light channels, the diameter of which is several millimeters, were determined. They are formed because of Kerr self-focusing of intensity inhomogeneities in the initial transverse profile of the laser beam. It is shown that the formation of a filament (a localized light structure, the existence of which is associated with the plasma formation and the generation of conical emission) does not occur in each of these channels. The theoretical evaluation of this light channels characteristics was carried out. It is based on the diffraction-ray model of single filamentation of femtosecond laser pulses. Studying of the evolution transverse profile of a laser beam with a centimeter radius and subterawatt power along air path showed that the initial radius of intensity inhomogeneities, for which laser filamentation occur, is equal several (2.5-3.5) millimeters. The power in these inhomogeneities varies from 19 to 26 GW. Differences in the values of the radius and power of these inhomogeneities are the cause of different distances from the laser pulse source at which their self-focusing occurs.
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