无反光镜光学参量振荡器中的相位调制传输

G. Stromqvist, V. Pasiskevicius, C. Canalias, C. Montes
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引用次数: 0

摘要

理论上已经预测[1],反向传播的参数相互作用,即信号和闲散波沿相反方向传播,将建立分布式反馈机制,从而在不需要使用反射镜或外部反馈腔的情况下实现光学参量振荡。这种装置,即无反光镜光学参量振荡器(MOPO),最近已经通过采用工程非线性晶体,即周期极化KTiOPO4 (PPKTP)实现,其结构周期为800 nm[2]。MOPO的一个显著特性是信号和闲散脉冲的频谱内容具有很强的不对称性,其中信号脉冲带宽与泵浦的带宽相同,而反向传播的闲散脉冲比信号窄约两个数量级。本文对MOPO的时间相转移特性进行了实验和理论研究。我们特别指出,相位调制主要转移到信号波,而空闲波几乎保持无相位调制。该特性允许在中红外光谱区域产生变换限制脉冲的简单方法,而不管泵的相位调制。理论仿真表明,空闲波中剩余的相位调制量取决于共传播泵浦波与信号波之间的群速度不匹配。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Phase modulation transfer in mirrorless optical parametric oscillators
It has been predicted theoretically [1] that counter-propagating parametric interactions, where the signal and idler waves are propagating in opposite directions, will establish a distributed feedback mechanism and thus optical parametric oscillation without the need to apply mirrors or external feedback cavity. Such a device, the mirrorless optical parametric oscillator (MOPO), has been recently realized by employing engineered nonlinear crystals, namely, periodically poled KTiOPO4 (PPKTP) with the periodicity of the structure of 800 nm [2]. One of the remarkable properties of the MOPO was a strong asymmetry in spectral content of the signal and idler pulses, where signal pulse bandwidth was of the same order as that of the pump while the counter-propagating idler was about two orders of magnitude narrower than the signal. In this work we provide experimental and theoretical investigation on the temporal phase transfer characteristics in MOPO. In particular we show that the phase modulation is transferred primarily to the signal wave while the idler wave remains almost phase-modulation-free. This property allows a simple means for generating transform-limited pulses in mid-infrared spectral region regardless of phase modulation of the pump. Theoretical simulation reveals that the amount of remaining phase modulation in the idler wave depends on the group-velocity mismatch between the co-propagating pump and signal waves.
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