Transient Measurements With A Photoconductively Gated Scanning Tunneling Microscope

U. Keil, J. R. Jensen, J. Hvam
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Abstract

For the combination of high spatial resolution with high temporal resolution we use a photoconductively gated scanning tunneling microscope (PGSTM). The instrument resolves voltage transients propagating on a coplanar waveguide (CPW) in space and time. In addition, we demonstrate the detection of laser induced field changes in a photoconductor. The setup, shown in Fig. I , differs in two aspects from previously reported designs.[ 1, 21 The tunneling tip is attached to a coplanar strip line providing direct electrical access to the tip. In addition, a fiber supplying the probe beam, is directly connected to the photoconductive (PC) switch which ensures an unconstrained positioning of the tip without variations in the illumination of the PC switch. The 100-fs laser source is split into a pump beam generating an electrical pulse on the sample and a probe beam gating the probe PC switch with a delay. Sample and probe substrates are low temperature grown (LT) GaAs and the PC switch response time is measured to be less than 1 ps. The current preamp controlling the feedback loop is connected to the tunneling tip through one electrode of the coplanar strip line. The other electrode is connected to an external preamp measuring the gated signal. Due to this modification we do not observe the previously reported linear dependence of the transient signal amplitude on the tunneling conductance.[ 13 The amplitude is independent of the tunneling resistance and decreases by a factor of four in a distance of 50 pm above the surface. All results can be explained by coupling through the geometrical capacitance of the tipelectrode gap. The instrument is used to map out the mode structure of voltage transients on transmission lines. Figure 2 shows a gray-scale contour plot of a pulse on a CPW generated
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光导门控扫描隧道显微镜的瞬态测量
为了实现高空间分辨率和高时间分辨率的结合,我们使用了光导门控扫描隧道显微镜(PGSTM)。该仪器在空间和时间上对共面波导上传播的瞬态电压进行了解析。此外,我们还演示了在光导体中检测激光诱导场变化的方法。图1所示的设置与先前报道的设计在两个方面不同。[1,21]隧道尖端连接在共面带状线上,提供对尖端的直接电通道。此外,提供探针光束的光纤直接连接到光导(PC)开关,这确保了尖端的不受约束的定位,而不会改变PC开关的照明。100-fs激光源被分成在样品上产生电脉冲的泵浦光束和延时控制探针PC开关的探针光束。样品和探针衬底为低温生长(LT) GaAs, PC开关响应时间小于1ps。控制反馈回路的电流前置放大器通过共面带状线的一个电极连接到隧道尖端。另一个电极连接到测量门控信号的外部前置放大器。由于这种修改,我们没有观察到先前报道的瞬态信号幅度与隧道电导的线性依赖关系。[13]振幅与隧道阻力无关,在离地表50pm的距离上下降了四倍。所有结果都可以通过尖端电极间隙的几何电容耦合来解释。该仪器用于绘制输电线路电压瞬态的模态结构。图2显示了生成的CPW上脉冲的灰度等高线图
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