Ultra-Short Pulse Modulation with Electro-Optic Modulators

Stefan Meyer, Tonio F. Kutscher, Philipp Lamminger, Florian Sommer, Sebastian Karpf
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Abstract

Multiphoton microscopy (MPM) is a promising technology for intravital imaging, providing deep tissue penetration, high 3D resolution and low photobleaching [1]. To realize MPM, it is crucial to make maximum use of the nonlinearity of the excitation probability by using high intensity laser illumination. Most often, this is achieved by using femtosecond pulses from a mode-locked laser, however, these pulses suffer from chromatic dispersion and unwanted nonlinearities. Recent research endeavours are exploiting picosecond pulses as pulse-on-demand alternatives [2], [3]. Here, we utilize a Mach-Zehnder-based intensity electro-optic modulator (EOM), which splits an optical beam in two partial beams and induces a phase modulation in one of the partial beams by means of an applied voltage [4]. Being waveguide-based, a small driving voltage of 5V (TTL levels) are required to achieve a $(V_{pi})$ full modulation between constructive and destructive interference. To achieve short picosecond pulses expensive electrical pulse generators are required to provide the short picosecond electrical pulses. In this work we report on a driving signal employing twice the $V_{pi}$ voltage to generate ultra short optical pulses. As shown in Fig. 1, using a voltage of $2V_{pi}$ causes the EOM to jump between two states of maximal suppression in the short time of the rising or falling edge (80/20-times of 35 ps shown) with a very short open state of the EOM in between.
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电光调制器的超短脉冲调制
多光子显微镜(MPM)是一种很有前途的活体成像技术,具有深层组织穿透、高3D分辨率和低光漂的特点[1]。利用高强度激光照射,最大限度地利用激发概率的非线性,是实现磁点法的关键。大多数情况下,这是通过使用锁模激光器的飞秒脉冲来实现的,然而,这些脉冲受到色散和不必要的非线性的影响。最近的研究工作是利用皮秒脉冲作为脉冲按需选择[2],[3]。在这里,我们利用基于马赫-曾德尔的强度电光调制器(EOM),它将光束分成两个部分光束,并通过施加电压在其中一个部分光束中诱导相位调制[4]。基于波导,需要5V (TTL电平)的小驱动电压来实现$(V_{pi})$在相消干涉之间的全调制。为了获得短皮秒脉冲,需要昂贵的电脉冲发生器来提供短皮秒电脉冲。在这项工作中,我们报告了使用两倍的$V_{pi}$电压来产生超短光脉冲的驱动信号。如图1所示,使用$2V_{pi}$的电压会导致EOM在上升沿或下降沿的短时间内(如图所示的35 ps的80/20倍)在两个最大抑制状态之间跳跃,其间EOM处于非常短的打开状态。
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