2004
DOI: 10.1143/jjap.43.4571
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Scanning Tunneling Microscopy Barrier Height Imaging of Subsurface Dopant Atoms on Hydrogen-Terminated Si(111)

Abstract: Dopant atoms beneath a hydrogen-terminated Si(111) 1×1 surface are investigated by scanning tunneling microscopy (STM) and barrier height (BH) imaging. Because of the weak screening effect of the hydrogen-terminated Si(111) surface, subsurface donors and acceptors can be imaged by STM. From BH images, we can deduce a local change in BH at subsurface dopant sites. Both the sign and magnitude of the observed BH change are in good agreement with calculations assuming a screened Coulomb potential for a dopant pote… Show more

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Cited by 4 publications
(10 citation statements)
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“…Consequently, the measured (dI/dZ) signal depends not only on the vacuum barrier height〈F〉but also on charge concentration Q S beneath the STM probe. The correlation of the (dI/dZ) signal to the surface charge density was conˆrmed by bias-dependent measurements on hydrogen-terminated Si(111) surfaces, 55,56) oxidized Si(110) surfaces 53) and cross sectional (001) surfaces of MOSFET devices. 41) Figure 6(a) shows line proles of the diŠerential conductance (dI/dZ) as a function of position across a drain extension for a cross section of a MOSFET device in Fig.…”
Section: Vacuum-gap Modulation Spectroscopymentioning
confidence: 96%
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“…Consequently, the measured (dI/dZ) signal depends not only on the vacuum barrier height〈F〉but also on charge concentration Q S beneath the STM probe. The correlation of the (dI/dZ) signal to the surface charge density was conˆrmed by bias-dependent measurements on hydrogen-terminated Si(111) surfaces, 55,56) oxidized Si(110) surfaces 53) and cross sectional (001) surfaces of MOSFET devices. 41) Figure 6(a) shows line proles of the diŠerential conductance (dI/dZ) as a function of position across a drain extension for a cross section of a MOSFET device in Fig.…”
Section: Vacuum-gap Modulation Spectroscopymentioning
confidence: 96%
“…One promising STM-based spectroscopy to investigate nanometer-scale roughness of electric interfaces in actual devices is vacuum-gap modulation (VGM) spectroscopy, also called barrier-height spectroscopy. 21,23,41,52,55,56) In this method, while the STM probe was scanning the sample, small modulation of the STM probe-sample gap was introduced at a frequency of 10-20 kHz with a small amplitude dZ of 20 pm by applying a sinusoidal voltage to the STM piezo-scanner. Current response dI was measured with a lock-in ampliˆer at each point of the topographical image.…”
Section: Vacuum-gap Modulation Spectroscopymentioning
confidence: 99%
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“…[9][10][11][12][13][14] Second, the close proximity of the STM tip near the surface induces localized band bendings, [15][16][17][18] which modify the potential around charged defects significantly and thus the screening cannot be probed quantitatively. Third, the limited signal to noise ratio of barrier height or surface photovoltage measurements [19][20][21] restrict a quantitative data analysis. These problems drastically limit the availability of reliable experimental data on screening at semiconductor surfaces.…”
Section: Introductionmentioning
confidence: 99%