空光学谐振腔内锁模态的转换

Michael Zwilich, Florian Schepers, C. Fallnich
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引用次数: 0

摘要

光学谐振器通常用作光谱分析仪或模式清除器[1],[2]。然而,正如这项工作所示,它们的光谱和空间滤波特性也可以用于将纵向锁模状态转换为横向锁模状态,反之亦然。对于纵向到横向转换,入射纵向锁模光束的光谱分量与空光学腔的横向模共振相匹配。因此,所有频谱分量同时传输并转换为横向模式。因此,调幅,即纵向锁模,梁被转换成横向锁模梁,在横向平面上快速振荡。这种转换方案允许分别控制锁定的横向模式及其各自的振幅,与在激光主动腔中激发横向锁模态相比,这改善了横向锁模态的产生[3]-[5]。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Conversion of Mode-Locked States within an Empty Optical Resonator
Optical resonators are routinely used as optical spectrum analyzers or mode-cleaners [1], [2]. However, as shown in this work, their spectral and spatial filtering properties can also be utilized to convert longitudinal to transverse mode-locked states and vice versa. For longitudinal to transverse conversion the spectral components of an incident longitudinal mode-locked beam are matched to transverse mode resonances of an empty optical cavity. As a result, all spectral components are transmitted simultaneously and converted into transverse modes. Thus, an amplitude-modulated, i.e. longitudinal mode-locked, beam is converted into a transverse mode-locked beam that rapidly oscillates across the transverse plane. This conversion scheme allows to control the set of locked transverse modes and their respective amplitudes separately, which improves the generation of transverse mode-locked states compared to their excitation in laser-active cavities [3]–[5].
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