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Possibility of carrier profiling semiconductors by terahertz spectroscopy with terahertz radiation generated in a scanning tunneling microscope

机译:通过在扫描隧道显微镜中产生的太赫兹光谱法通过太赫兹光​​谱法产生载体分析半导体的可能性

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A mode-locked ultrafast laser focused on the tunneling junction of a scanning tunneling microscope (STM) superimposes harmonics of the laser pulse repetition frequency on the DC tunneling current. The power measured at each of the first 200 harmonics (up to 15 GHz) varies inversely as the square of the frequency due to stray capacitance shunting the tunneling junction. Fourier analysis suggests that in the tunneling junction the harmonics have no significant decay up to a frequency of 1/2τ ≈ 33 THz where τ = 15 fs, the laser pulse width. Two different analyses will be presented to model the generation of the frequency comb within the tunneling junction. The first is based on the observed current-voltage characteristics for the nanoscale tunneling junction. The second is a solution of the time-dependent Schr?dinger equation for a modulated barrier. Both analyses indicate that optical rectification of the pulsed laser radiation in the tunneling junction causes harmonics of the pulse repetition frequency of the laser and that these harmonics may extend to terahertz frequencies. It appears that the tunneling junction may be used as a sub-nm sized source of terahertz radiation. Transmission and back scattering could not be used but loading of this source by the finite conductivity of the semiconductor would cause a loss varying inversely with the carrier density. Carrier dynamics could be measured by time-domain measurements, and time-averaged carrier profiling, but presumably with finer resolution due to the sub-nm size of the terahertz source.
机译:一种锁定的超快激光器,聚焦在扫描隧道显微镜(STM)的隧道结叠加在DC隧道电流上的激光脉冲重复频率的谐波。在前200次谐波(最多15GHz)中测量的功率在频率旋转隧道连接处的频率方面变化成反比地变化。傅立叶分析表明,在隧道结中,谐波没有显着衰减到1 /2τ≈33Thz的频率,其中τ= 15 fs,激光脉冲宽度。将提出两种不同的分析来模拟隧道连接内的频率梳的产生。首先是基于纳米级隧道结的观察电流电压特性。第二种是调制屏障的时间依赖性SCHR的解决方案。两种分析表明隧道结中脉冲激光辐射的光学整流导致激光脉冲重复频率的谐波,并且这些谐波可以延伸到太赫兹频率。似乎隧道连接可以用作太赫兹辐射的亚NM尺寸源。不能使用传动和后散射,但是通过半导体的有限电导率加载该来源将导致载流子密度反向变化的损失。可以通过时域测量和时间平均载波分析来测量载波动态,但由于太赫兹源的子NM大小,可能具有更精细的分辨率。

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