TY - JOUR
T1 - Surface potential mapping in the SiO2 system using a FET cantilever
AU - Suh, Moon Suhk
AU - Lee, Churl Seung
AU - Kim, Sung Hyun
AU - Lee, Kyoung Il
AU - Cho, Jin Woo
AU - Choi, Young Jin
AU - Shin, Jin Koog
N1 - Funding Information:
This work was supported by National R&D Project for Nano Science and Technology.
Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2006/8
Y1 - 2006/8
N2 - The surface potential variations are measured, according to the enhanced measuring speed and voltage sensitivity, using an active device, such as a field-effect-transistor (FET) [R.C. Barrett, C.F. Quate, J. Appl. Phys. 70 (1991) 2725; Y. Martin, D.W. Habraham, H.K. Wickramasighe, Appl. Phys. Lett. 52 (1988) 1103; G.H. Buh, H.J. Chung, Y. Kuk, Appl. Phys. Lett. 79 (2001) 2010]. In this study, the surface potential was mapped in the patterned SiO2 medium at room temperature. An improved FET-tip cantilever, which has a source, a drain, and an n-channel, was used in this study. The potential images were analyzed both in the contact mode and the non-contact mode, using only a pre-amplifier system instead of a lock-in the amplifier. A probe was used to measure the surface potential with a resolution of <100 nm in the contact mode operation, based on the edge of the patterned SiO2 islands. In the non-contact mode, however, the resolution of the surface potential was measured at about 270 nm at low scanning speed. The probe can also be used to write charges on a surface.
AB - The surface potential variations are measured, according to the enhanced measuring speed and voltage sensitivity, using an active device, such as a field-effect-transistor (FET) [R.C. Barrett, C.F. Quate, J. Appl. Phys. 70 (1991) 2725; Y. Martin, D.W. Habraham, H.K. Wickramasighe, Appl. Phys. Lett. 52 (1988) 1103; G.H. Buh, H.J. Chung, Y. Kuk, Appl. Phys. Lett. 79 (2001) 2010]. In this study, the surface potential was mapped in the patterned SiO2 medium at room temperature. An improved FET-tip cantilever, which has a source, a drain, and an n-channel, was used in this study. The potential images were analyzed both in the contact mode and the non-contact mode, using only a pre-amplifier system instead of a lock-in the amplifier. A probe was used to measure the surface potential with a resolution of <100 nm in the contact mode operation, based on the edge of the patterned SiO2 islands. In the non-contact mode, however, the resolution of the surface potential was measured at about 270 nm at low scanning speed. The probe can also be used to write charges on a surface.
KW - AFM
KW - Cantilever
KW - Contact mode
KW - FET
KW - Non-contact mode
KW - Surface potential
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U2 - 10.1016/j.cap.2006.01.045
DO - 10.1016/j.cap.2006.01.045
M3 - Article
AN - SCOPUS:33746218179
SN - 1567-1739
VL - 6
SP - e224-e231
JO - Current Applied Physics
JF - Current Applied Physics
IS - SUPPL. 1
ER -