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Open loop Kelvin probe force microscopy with single and multi-frequency excitation
Date Issued
2013-11-29
Date Available
2014-11-30T04:00:13Z
Abstract
Conventional Kelvin probe force microscopy (KPFM) relies on
closed loop (CL) bias feedback for the determination of surface
potential (SP). However, SP measured by CL-KPFM has been shown to be
strongly influenced by the choice of measurement parameters due to
non-electrostatic contributions to the input signal of the bias feedback
loop. This often leads to systematic errors of several hundred mV and
can also result in topographical crosstalk. Here, open loop (OL)-KPFM
modes are investigated as a means of obtaining a quantitative, crosstalk
free measurement of the SP of graphene grown on Cu foil, and are
directly contrasted with CL-KPFM. OL-KPFM operation is demonstrated in
both single and multi-frequency excitation regimes, yielding
quantitative SP measurements. The SP difference between single and
multilayer graphene structures using OL-KPFM was found to be 63 ± 11 mV,
consistent with values previously reported by CL-KPFM. Furthermore, the
same relative potential difference between Al2O3-coated graphene and Al2O3-coated
Cu was observed using both CL and OL techniques. We observed an offset
of 55 mV between absolute SP values obtained by OL and CL techniques,
which is attributed to the influence of non-electrostatic contributions
to the input of the bias feedback used in CL-KPFM.
closed loop (CL) bias feedback for the determination of surface
potential (SP). However, SP measured by CL-KPFM has been shown to be
strongly influenced by the choice of measurement parameters due to
non-electrostatic contributions to the input signal of the bias feedback
loop. This often leads to systematic errors of several hundred mV and
can also result in topographical crosstalk. Here, open loop (OL)-KPFM
modes are investigated as a means of obtaining a quantitative, crosstalk
free measurement of the SP of graphene grown on Cu foil, and are
directly contrasted with CL-KPFM. OL-KPFM operation is demonstrated in
both single and multi-frequency excitation regimes, yielding
quantitative SP measurements. The SP difference between single and
multilayer graphene structures using OL-KPFM was found to be 63 ± 11 mV,
consistent with values previously reported by CL-KPFM. Furthermore, the
same relative potential difference between Al2O3-coated graphene and Al2O3-coated
Cu was observed using both CL and OL techniques. We observed an offset
of 55 mV between absolute SP values obtained by OL and CL techniques,
which is attributed to the influence of non-electrostatic contributions
to the input of the bias feedback used in CL-KPFM.
Sponsorship
Science Foundation Ireland
Other Sponsorship
UCD Research
Programme for Research in Third Level Institutions Cycle 5
European Regional Development Fund
Alexander von Humboldt Foundation
Zurich Instruments
Type of Material
Journal Article
Publisher
Institute of Physics
Journal
Nanotechnology
Volume
24
Issue
47
Start Page
475702
Copyright (Published Version)
2013 IOP Publishing
Language
English
Status of Item
Peer reviewed
This item is made available under a Creative Commons License
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Collins_et_al_Nanotechnology_2013.pdf
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