Optical fibres with sharp discontinuities as intracavity mode-locking devices for ultrashort-pulse fibre ring lasers

E. Romanova, E. Bekker, L. Melnikov
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Abstract

1. In a Ken-lens mode-locking (KLM) resonator (Fig. la) for femtosecond pulse generation, the self-focusing effect within a Ken medium (KM) modifies the cavity mode profile. This is described as a self-amplitude modulation resulting in either decreasing loss through an internal aperture as the field intensity increases (hard aperturing) or increasing gain by adjusting the overlap between the cavity and the pump mode profiles (soft aperturing). Because the KLM uses bulk nonlinearities, it is well suited for mode-locking bulk solid-state lasers which have high intracavity intensities [l]. In fibre lasers, where nonlinear phase shifts are integrated over the fibre length, the additive pulse mode-locking (APM) is used. Polarisation APM (P-APM) relies on the intensity-dependent rotation of the elliptical polarisation state in a length of optical fibre. With proper settings of the initial polarization ellipse and phase bias, pulse shortening occurs. Optical fibre is well suited for nonlinear polarization rotation because the small mode diameter leads to high intensities and thus to a large nonlinear index change, and because long fibre length can be used. Unidirectional fibre ring cavity has low self-starting threshold. It can operate in the soliton regime, where the group velocity dispersion is negative, or in the stretched pulse regime (Fig. 1 b), where sections of both positiveand negative-dispersion fibre are used [ 2 ] . However polarization elements are sensitive to thermal and mechanical environmental changes. As an alternative to the polarization mode-locking devices, we suggest to use fibre discontinuities to achieve KLM operation in the fibre ring lasers. Step-like discontinuity in a fibre loop can be considered as an analog to a hard aperture inside linear resonator of the KLM laser. In our previous works, we have demonstrated applicability of the step-like discontinuities for pulse compression in optical fibres [3]. In this paper, mode-locking action of the both polarization rotator and step-like discontinuity is evaluated depending on parameters of the devices and compared. Ultra-short pulse propagation through nonlinear fibre segments is simulated numerically with account of material dispersion and gain in the fibre loop.
作为超短脉冲环形光纤激光器腔内锁模装置的尖锐不连续光纤
1. 在用于飞秒脉冲产生的肯透镜锁模(KLM)谐振器(图la)中,肯介质(KM)内的自聚焦效应改变了腔模式轮廓。这被描述为一种自振幅调制,通过内部孔径随着场强度的增加而减少损耗(硬孔径)或通过调整腔和泵浦模式轮廓之间的重叠来增加增益(软孔径)。由于KLM采用了体非线性,因此它非常适合于具有高腔内强度的锁模体固体激光器[1]。在光纤激光器中,非线性相移在光纤长度上进行积分,使用加性脉冲锁模(APM)。偏振APM (P-APM)依赖于一段光纤中椭圆偏振态的强度依赖旋转。通过适当设置初始偏振椭圆和相位偏置,可以使脉冲缩短。光纤非常适合于非线性偏振旋转,因为小的模直径导致高强度,从而导致大的非线性折射率变化,因为长纤维长度可以使用。单向纤维环腔自启动阈值低。它可以在群速度色散为负的孤子状态下工作,也可以在拉伸脉冲状态下工作(图1b),其中使用了正色散和负色散光纤的部分[2]。然而,极化元件对热环境和机械环境的变化非常敏感。作为偏振锁模装置的替代方案,我们建议在光纤环形激光器中使用光纤不连续点来实现KLM操作。光纤环路中的阶跃不连续可以看作是KLM激光器线性谐振腔内硬孔的类比。在我们之前的工作中,我们已经证明了在光纤中脉冲压缩的阶梯状不连续的适用性[3]。本文根据器件参数对极化旋转器和步进不连续器的锁模作用进行了评价和比较。考虑光纤环路中材料色散和增益的影响,对超短脉冲在非线性光纤段中的传播进行了数值模拟。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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