Self-sustained Picosecond Pulse Generation in a GaAlAs Laser at an Electrically Tunable Repetition Rate

K. Lau, A. Yariv
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引用次数: 40

Abstract

Picosecond pulse generation from semiconductor lasers at high repetition rate is generally accomplished by two different means: mode-locking or direct electrical excitation. The shortest ever pulses of below lps was generated from a passively mode-locked GaAlAs laser [1], while active mode-locking produces somewhat longer optical pulses. The pulse repetion rate of the mode-locked laser is determined by the length of the external cavity and cannot be varied easily. The rather critical optical alignment necessary for operating the laser in an external cavity makes these mode-locked semiconductor lasers somewhat inconvenient in practical applications. A second means of picosecond pulse generation is by directly pumping the laser with intense, short electrical pulses [2,3] or by large amplitude sinusoidal current modulation [4,5]. Optical pulses generated by such means have pulse widths in the vicinity of 15-35 ps. This scheme requires an external RF source for exciting the laser. In this work, we will show that by using a state-of-the-art high speed laser in the optoelectronic feedback configuration shown in Fig. 1, highly stable optical pulses (with jitters of <10fs), with pulse widths between 10 and 20 ps can be generated, with a very high repetition rate from 1 5GHz which can be electrically tuned. This scheme has the advantage of eradicating the necessity of any external RF drive and/or sensitive optical alignment.
电可调重复频率下GaAlAs激光器中自维持皮秒脉冲的产生
高重复率半导体激光器产生皮秒脉冲通常通过两种不同的方式实现:锁模或直接电激励。被动锁模GaAlAs激光器[1]产生的脉冲最短,而主动锁模激光器[1]产生的脉冲较长。锁模激光器的脉冲重复率由外腔的长度决定,不易改变。在外部腔中操作激光器所必需的相当关键的光学对准使得这些锁模半导体激光器在实际应用中有些不方便。皮秒脉冲产生的第二种方法是直接用强而短的电脉冲泵送激光[2,3]或通过大振幅正弦电流调制[4,5]。通过这种方法产生的光脉冲的脉冲宽度在15- 35ps附近。该方案需要一个外部射频源来激发激光。在这项工作中,我们将展示通过在图1所示的光电反馈配置中使用最先进的高速激光器,可以产生高度稳定的光脉冲(抖动<10fs),脉冲宽度在10到20 ps之间,具有非常高的重复率,从15 ghz可以电调谐。该方案的优点是消除了任何外部射频驱动和/或敏感光学校准的必要性。
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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