2008
DOI: 10.1063/1.2888733
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Probing nanoscale potential modulation by defect-induced gap states on GaAs(110) with light-modulated scanning tunneling spectroscopy

Abstract: We investigated charged defects on an n-GaAs͑110͒ surface using light-modulated scanning tunneling spectroscopy. Tunneling via a single defect-induced gap state under photoillumination was observed for the isolated atomic defects. Screened Coulomb potentials induced around a charged Ga vacancy and a step edge were visualized, for the first time, with a nanometer spatial resolution. Furthermore, the charge states of the individual defects were determined on the atomic level.

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Cited by 18 publications
(25 citation statements)
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“…First, the I-V s curve in the dark for GaAs (blue line in Figure 3(b)) reveals that the tunneling current does not flow unless a bias voltage much larger than the bandgap energy is applied. This is because large TIBB occurs at both positive and negative bias voltages [20,[22][23][24][25]. This tendency is also present for AlGaAs and LT-GaAs (Figures 3(c) and 3(d)).…”
Section: Band Structure Investigated By Lm-stssupporting
confidence: 50%
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“…First, the I-V s curve in the dark for GaAs (blue line in Figure 3(b)) reveals that the tunneling current does not flow unless a bias voltage much larger than the bandgap energy is applied. This is because large TIBB occurs at both positive and negative bias voltages [20,[22][23][24][25]. This tendency is also present for AlGaAs and LT-GaAs (Figures 3(c) and 3(d)).…”
Section: Band Structure Investigated By Lm-stssupporting
confidence: 50%
“…This indicates that no photocarriers are generated and the AlGaAs layer works well as a barrier against the flow of photocarriers from the adjacent LT-GaAs and GaAs layers, as expected. If photocarriers had flowed from GaAs or LT-GaAs into AlGaAs, TIBB in AlGaAs would have been reduced, as observed at the pn junction of GaAs in previous studies [23][24][25]. The slight changes seen in the red and blue curves in Figure 3(c) are due to the effect of photovoltage at the LT-GaAs/AlGaAs/GaAs interfaces, which will be discussed in Section 3.4.…”
Section: Band Structure Investigated By Lm-stsmentioning
confidence: 70%
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“…The addition of optical technologies to STM provides new approaches to the study of nanoscale-material physics and chemistry. Nearfield optical microscopy (NSOM) and other techniques [78][79][80][81][82][83][84][85][86], which have not been discussed in this chapter, are expected to play complementary roles in understanding and developing the physics and chemistry of new nanoparticles/clusters for realizing novel functional devices.…”
Section: Discussionmentioning
confidence: 99%
“…Quantitative potential measurements rely on a statistical analysis of interacting charged defects, 19,20,26 the band edge determination in tunneling spectra, 4,14 a work function measurement, or surface photo voltage measurements. 27 However, in the latter two cases, the tip-induced band bending severely affects the results by shifting the band edges. [28][29][30][31] This band edge shift is not homogeneous across the surface, because the screening ability varies spatially, e.g., with the fluctuations in the dopant distribution or the material across heterointerfaces.…”
Section: Introductionmentioning
confidence: 99%