Theoretical study of dispersive wave generation in ar-filled hollow-core PCF above the plasma threshold

W. Chang, A. Nazarkin, J. Travers, P. Holzer, J. Nold, N. Y. Joly, P. Russell
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Abstract

Hollow-core photonic-crystal fibre (HC-PCF) [1] provides a highly efficient means for investigating light-matter interactions at sustained intensity levels inaccessible to both traditional bulk setups (due to limited interaction lengths) or conventional optical fibres (due to the low damage threshold of glass). Recent experiments have shown that strong UV pulses can be generated, through emission of dispersive radiation, by launching near-IR femtosecond pulses into a gas-filled kagomé-lattice PCF [2]. Phase-matching to the UV can be accounted for through the special dispersion characteristics of the gas-filled HC-PCF [3]. Shorter UV wavelengths require higher energy pulses, causing the intensity to enter the ionisation regime when pulse propagation will be influenced by the presence of free electrons. The transition from the “traditional” regime where the Kerr effect dominates to the plasma regime where ionisation becomes important (novel in the context of photonic crystal fibres) is studied numerically in this work.
等离子体阈值以上充ar空心芯PCF中色散波产生的理论研究
空心光子晶体光纤(HC-PCF)[1]提供了一种高效的方法来研究光-物质相互作用的持续强度水平,这是传统的块体装置(由于相互作用长度有限)或传统光纤(由于玻璃的低损伤阈值)无法实现的。最近的实验表明,通过发射色散辐射,将近红外飞秒脉冲发射到充满气体的kagomacom -lattice PCF中,可以产生强紫外脉冲[2]。通过充气HC-PCF的特殊色散特性,可以解释与UV的相位匹配[3]。较短的紫外波长需要较高的能量脉冲,当脉冲传播将受到自由电子存在的影响时,导致强度进入电离状态。从克尔效应占主导地位的“传统”状态到电离变得重要的等离子体状态(在光子晶体光纤的背景下是新颖的)的转变在本工作中进行了数值研究。
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