基于等离子体基太赫兹源焦区尺寸的脉冲展宽效应

T. Shen, H. Wang, J. Zhang, J. Liu
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引用次数: 0

摘要

太赫兹产生机理的研究一直存在一个问题。实验中泵浦激光脉冲持续时间在飞秒量级,而辐射太赫兹脉冲持续时间达到皮秒量级。在光导天线法中,它被解释为载流子动量的松弛。对于基于等离子体的太赫兹辐射,我们认为激光脉冲的空间传播是造成这种现象的原因。对于长脉冲,脉冲长度远大于聚焦区域;因此,可将焦点区域视为一个点,并应采用经典击穿模型。当脉冲持续时间接近飞秒时,脉冲不会填充整个焦区域,而是在任何给定时刻仅占焦区域的一小部分;因此,应采用飞秒击穿模型。该模型可以解释太赫兹产生中的脉冲展宽现象。然而,从空间的角度来看,它表明了某种频率转换。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Pulse Broadening Effect Based on the Focal Region Size in Plasma-Based Terahertz Sources
There is an issue throughout the research of the THz generation mechanism. The pump laser pulse duration in the experiment is on the order of femtoseconds, but the radiated THz pulse duration reaches the order of picoseconds. [1] It is interpreted as relaxation of carrier momentum in the photoconductive antenna method. [2] As for the plasma-based THz radiation, we believe that the spatial propagation of the laser pulse is responsible for this phenomenon. For a long pulse, the pulse length is much larger than the focal region; hence, the focal region can be treated as a point and classical breakdown model should be employed. When the pulse duration approaches the femtosecond regime, the pulse will not fill the entire focal region and instead occupies only a small fraction of the focal region at any given instant; Thus, a femtosecond breakdown model should be employed. [3] This model can explain the pulse broadening phenomenon in the terahertz generation. However, it indicates some kind of frequency conversion from a spatial perspective.
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