■ Principle of SKPM op
Kelvin Force Microscopy (KFM) is designed to observe a surface-potential image of a
specimen by detecting the electrostatic force generated between a cantilever and a
specimen using an AC-mode atomic force microscope (AFM) and controlling the bias
potential of the specimen so that the electrostatic force becomes a minimum.
The following states the principle of KFM.
If U is the potential difference between a cantilever and a specimen, the electrostatic
force generated between them is given by the following equation:
Here, z is the distance between the cantilever and the specimen, and C is the electrostatic
capacitance. An AC voltage with amplitude V
on DC voltage V
This superposed voltage is applied between the cantilever and the specimen. If the
contact potential difference is ∆ φ/q
Fr
om the above equati
This equation can be expanded
The
Electrostatic force F has both a static component and components at angular
frequ
encies ω and 2 ω , as shown in
change of the vibration amplitude (F: Force) of the cantilever and the charac
frequ
ency (
Lock-in Amplifier. In the case of Force, the ω component corresponds to
∂
C
(
⋅
−
V
DC
∂
z
In the case of Force gradient the ω component corresponds to
The specimen surface potential is measured by controlling
beco
mes zero.
• RE
FERENCE:
Hiroshi Yokoyama, et al., Journal of The Physical Society of
T. Hochwitz, et al., Journal of V
∗
∆φ(units: eV
) is the Work Function Difference (WFD) and ∆φ/q(units: V) is the Contact Potential Difference
(CPD).
TMPM5200-2
eration
∂
1
C
=
−
⋅
2
⋅
F
U
z ∂
2
is given by the following equation:
DC,
=
+
⋅
V
V
V
t
DC
AC
φ
=
−
∆
U
V
/
q
t
t
φ
−
∆
+
⋅
V
/
q
V
s
in
DC
AC
on, the el
ectrostatic force F is given as follows:
1
(
φ
=
−
⋅
−
∆
+
F
V
/
q
DC
2
as follows:
⎡
1
(
φ
=
−
⋅
−
∆
F
V
/
q
⎢
DC
2
⎣
∂
C
(
)
φ
−
⋅
−
∆
⋅
V
/
q
V
DC
∂
z
∂
1
C
2
ω
+
⋅
⋅
⋅
V
cos
2
AC
∂
4
z
∂
F
: Z-component of Force gradient). The ω component is removed using the
∂
z
)
, as shown in the second term of equation (1).
φ
∆
⋅
/
q
V
AC
and angular frequency ω , superimposed
AC
ω
sin
t
∗
, the potential difference U is :
ω
t
∂
C
)
ω
2
⋅
⋅
V
sin
t
AC
∂
z
∂
⎤
1
C
)
2
2
+
⋅ ⎥
V
AC
∂
2
z
⎦
ω
⋅
sin
t
AC
(1)
t
equation (1). These components are detected as the
acuum Science Technology, B14,
5 MEASUREMENT OPERATION
t
2
∂
C
(
)
φ
⋅
−
∆
V ⋅
V
/
q
DC
AC
∂
2
z
V
so that this
DC
Japan, 49, 281 (1994)
457 (1996)
teristic
.
value
5-75
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