NT-MDT Solver Next - Scanning

7
H
d
i
S
t
S
c
(t
h
p
a
T
o
(
s
T
h
●
7
.3.1.4.
H
ereafter, t
h
i
sk.
t
artin
g
me
a
c
anning of
h
e sample
h
a
rameters h
o
start sca
n
s
ee Fig. 7-7
9
h
is results i
Line-by-
l
appear i
n
taken wi
t
the seco
n
displays
d
sample s
u
Fi
g
Scanni
n
h
e scanning
a
surement
s
the sampl
e
h
as approa
c
ave been s
e
n
ning, clic
k
9
).
F
n the follo
w
l
ine scanni
n
n
the 2D V
i
t
h the Sens
H
n
d one sh
o
d
istributio
n
u
rface ( Pha
g
. 7-80. Ima
g
of the Z
-
n
g
process
w
s
e
surface s
h
c
hed to the
e
t).
k
the Run
F
ig. 7-79. Co
w
ing activit
y
n
g of the s
a
i
ewer of th
H
ei
g
ht sig
n
o
ws variati
o
n
of the z-c
o
se signal)
(
g
es of surfa
c
-
component
o
on the
s
w
ill be expl
a
h
ould be pr
e
probe, the
b
utton in
t
ntrol panel
o
y
of the sys
a
mple surf
a
e scan dat
a
n
al (the first
o
ns at the
o
mponent
o
(
see Fig. 7-
6
c
e topograp
h
o
f the magn
e
s
urface of a
m
C
a
ined with
e
ceded by
n
operation
p
t
he Control
o
f the Scann
te
m
:
a
ce starts a
n
a
. Two of t
h
one uses s
c
backward
f the gradi
e
6
6);
h
y (upper pa
r
e
tic forces g
r
m
agnetic ha
r
C
hapter 7. P
e
the examp
l
n
ecessary
p
p
oint is adj
u
panel of
t
in
g
window
n
d three i
m
h
ese image
c
an in the f
o
movement
)
e
nt of the
m
r
t) and spati
a
r
adient (low
e
r
d disc
e
rforming M
e
l
e of a ha
r
p
reparation
u
sted, and
a
t
he Scanni
n
m
ages of th
e
s reveal th
e
fo
rward dir
e
)
and the
t
m
agnetic fo
r
a
l distributio
n
e
r part)
e
asurement
s
10
9
d magneti
c
procedure
s
a
ll scannin
g
ng
windo
w
e
scan are
a
e
landscap
e
e
ction whil
e
t
hird imag
e
r
ce over th
e
n
s
9
c
s
g
w
a
e
e
e
e