Generation of Pulsed Fiber Laser: ns to fs domain

M. Pal, S. D. Chowdhury, Nishant Kumar Shehar, R. Sen
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Abstract

Recently fiber lasers have become an indispensable tool in scientific endeavors as well as in multifarious industrial applications. While high power continues wave fiber lasers delivering hundreds of watts to killo-watts of average power are being used in manufacturing and strategic sectors for cutting, welding, additive manufacturing and directed energy applications, pulsed fiber lasers operating in the kHz repetition rate and nano-second pulse duration with pulse energies from micro-joule to mille-joule are being used for marking and engraving applications. These pulses are usually obtained from a Q-switched master oscillator power amplifier (MOPA) fiber laser or by amplifying a gain-switched laser diode to suitable pulse energy and power. Apart from this class of pulsed fiber lasers, mode-locked fiber lasers which now a days can deliver a very large variety of pulse duration ranging from femto-seconds to micro-seconds, are used for more precise and novel applications such as marking/ engraving on reflecting/ transmitting materials, nonlinear wavelength conversion, label free nonlinear microscopy, novel pump sources and also for study of various pulse dynamics [1, 2].
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脉冲光纤激光器的产生:ns到fs域
近年来,光纤激光器已成为科学研究和各种工业应用中不可或缺的工具。高功率连续波光纤激光器提供数百瓦至千瓦的平均功率,被用于制造和战略部门,用于切割、焊接、增材制造和定向能应用,脉冲光纤激光器以kHz重复率和纳秒脉冲持续时间工作,脉冲能量从微焦耳到千焦耳,被用于打标和雕刻应用。这些脉冲通常从调q主振荡器功率放大器(MOPA)光纤激光器或通过增益开关激光二极管放大到合适的脉冲能量和功率来获得。除了这类脉冲光纤激光器外,锁模光纤激光器现在可以提供从飞秒到微秒的各种脉冲持续时间,用于更精确和新颖的应用,例如在反射/传输材料上打标/雕刻,非线性波长转换,无标签非线性显微镜,新型泵浦源以及各种脉冲动力学的研究[1,2]。
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