NT-MDT Solver Next - Kelvin Probe Microscopy

Solver NE
X
110
●
The R
e
(see Fi
g
Should th
e
NOTE. D
u
signal coll
How to i
m
When the
defaults.
T
parameter
s
∆ Z
Amp
Other ru
n
“Scanning
”
7.3.2.
7.3.2.1.
Kelvin Pr
potentials.
electric fi
e
proper dc
b
X
T SPM. Inst
r
e
start
b
utt
o
g
. 7-81).
Fig. 7-81.
C
e
scanning
p
u
ring the se
c
ected at th
e
m
prove the
MFM mo
d
T
he acquire
d
s
:
probe-sur
fa
smaller is
e
pass. Ho
w
probe asc
e
panel of t
h
amplitude
amplitude
worsens t
h
of the Int
e
Operation
s
n
-time ope
r
”
on p. 97.
Kelvin
P
Brief
D
obe Micro
This techn
i
e
lds at the r
e
b
ias U
0
is a
p
r
uction Man
u
o
n becomes
C
ontrol panel
p
rocedure b
e
c
ond pass,
i
e
first pass.
ima
g
e
d
e is sele
c
d
image ca
n
fa
ce distanc
e
e
ffect of th
e
w
ever, incre
a
e
nt (sample
h
e Scannin
g
of the gen
e
of the pro
b
h
e signal/no
e
ractive Bl
o
s
panel and
r
ations on
P
robe M
D
escript
i
scop
y
(SK
M
i
que uses t
h
e
sonance fr
p
plied to th
e
u
al
enabled a
n
of the Sca
n
e
interrupte
i
nput of the
f
c
te
d
, the p
a
n
be impro
v
e
(offset) k
e
e
landscap
e
a
se of the
o
descent) i
s
g
window.
e
rator outp
u
b
e oscillati
ise ratio. T
o
o
ck Schem
e
enter the d
e
adjusting
icrosco
p
i
on
M
) is a tec
h
h
e effect th
a
equency) i
n
e
probe.
n
d caption
n
ning windo
w
d, click the
f
eedback i
s
a
rameters
o
v
ed with
r
u
e
pt during
t
e
variation
o
o
ffset redu
c
s
defined i
n
u
t. Reducin
g
on) impro
v
o
modify t
h
e
with the
e
sired valu
e
the para
m
p
y
h
ni
q
ue to s
a
t amplitud
e
n
the electri
of the Run
w
in the cou
r
Stop
b
utto
n
s
taken fro
m
o
f the seco
n
u
n-time adj
u
t
he second
o
n the dete
c
c
es sensitiv
i
n
the ∆ Z i
n
g
the gener
a
v
es sensiti
v
h
e Amp par
a
e
in the
A
m
p
m
eters are
tudy distri
b
e
of the pro
b
c field of t
h
b
utton ch
a
r
se of scann
i
n
or use th
e
m
the profil
e
n
d pass ar
e
u
stment of
pass. The l
a
c
tion signal
i
ty of the t
e
n
put field o
a
tor output
v
ity of the
t
a
meter, ope
b
utto
n
p
input fiel
d
explained
b
ution of s
u
b
e oscillati
o
h
e surface i
s
a
nges to St
i
ng
e
<Esc> ke
y
e
of the Se
n
e
set to th
the followi
a
rger ∆ Z ,
t
of the seco
e
chnique.
T
n the Cont
r
(and thus
t
t
echnique
b
n the wind
o
n
in the M
a
d
.
in i. 7.2.
1
u
rface elect
r
o
n (excited
s
zero whe
n
op
y
.
n
s
Z
eir
ng
t
he
nd
T
he
r
ol
t
he
b
ut
o
w
a
in
1
.6
r
ic
by
n
a