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University of Twente
Systems and Materials for Information storage
Magnetic Force Microscopy
Leon Abelmann and Martin SiekmanSystems and Materials for Information storage
MESA+ Research Institute
University of Twente
Constanta Summerschool, Sep 2005 (September 14, 2005)
Introduction 2,2(2)
Contents
• Before break: MFM Operation� Principle of MFM� MFM tips
• After break:� Instrumentation� Artefacts
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 1
Principle of MFM 5,5(3)
Principle of MFM
3 dimensionalScanner
Cantilever
Specimen
DetectorMagnetic element
z
xy
ComputerControlElectronics
M
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 2
Principle of MFM 7,7(2)
Magnetic Force Microscopy
500 nm
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 3
Principle of MFM 12,12(5)
Change in resonance
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 4
Principle of MFM 15,15(3)
Amplitude, Phase, Frequency
0
0
-180
-90
Phas
e di
ffer
ence
[deg
]A
mpl
itud
e [n
m]
Drive frequency [Hz]fres fres
,
phase
frequency
amplitude
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 5
Principle of MFM 18,18(3)
Image formation
Transform stray field to Fourier space:
H(kx, ky, z) =∫ ∞
−∞
∫ ∞
−∞H(x, y, z)e−i(xkx+yky)dxdy
H(kx, ky, z) = exp(−|k|z) · H(kx, ky, 0)
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 6
Principle of MFM 28,0(10)
MFM Demonstrator
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 7
Principle of MFM 31,3(3)
Tip transfer function
l
non-magnetic bar
magnetic coating
s
h
b
z0x0
t
10
12.5
1.25
0.13
125
1
0.1
10201002001000
0.01
0.001
810
710
610
510
Forc
e d
eriv
ativ
e [m
N/m
] Freq
uenc
y shift [Hz]
-1Spatial frequency [m ]
Wavelength l [nm]
Fz(k, z) = −µ0Mt · b sinc(kxb
2) · S sinc(
kyS
2) · H(k, z)
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 8
Principle of MFM 41,0(10)
MFM Demonstrator 2
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 9
Principle of MFM 51,10(10)
Resolution versus distance
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 10
MFM Probes 53,12(2)
Probes
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 11
MFM Probes 55,14(2)
AFM sputtered
�
• Sputtered CoCr(X) hard disk materials• Low/high moment: layer thickness• Fe, NiFe for low coercivity tips
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 12
MFM Probes 57,16(2)
AFM side coated
�
• Co, NiFe evaporated• Shape anisotropy• Stable domain structure
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 13
MFM Probes 59,18(2)
CantiClever
Tip plane
Cantilever
MFM tip
Cross-section determined by layer thicknessesLeon Abelmann Constanta Summerschool, Sep 2005 Slide 14
MFM Probes 61,20(2)
SEM Images cantilever
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 15
MFM Probes 63,22(2)
SEM Images tip
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 16
Break 0,0(0)
Break
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 17
Instrumentation 2,2(2)
Beam Deflection
�����
�������
• Laser• LED
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 18
Instrumentation 4,4(2)
Interferometer���������� ��������
• factor 10 better sensitivity• difficult to align• better reflection coatings
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 19
Instrumentation 7,7(3)
Thermal Noise
(∆
(∂F
∂z
)th
)rms
=
√4kTc∆B
ωnQ〈z2osc〉
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 20
Instrumentation 10,10(3)
Drift
1/Dt1/(NDt)
frequency (Hz)
Noi
se (n
m o
r H
z)
DB
DB’
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 21
Instrumentation 13,13(3)
Vacuum
• Reduce damping, improves Q-factor by 105
• Sound isolation
• Remove most of water film (meniscus)
Be careful with break-down (Paschen curve)
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 22
Instrumentation 16,16(3)
Magnetic Field
Application of magnetic fields
• On sample� Simple� Only in-plane� Low field� Heating
• On microscope� Requires very small microscope
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 23
Instrumentation 18,18(2)
Instrumentation
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 24
Instrumentation 20,20(2)
Switching Field Distribution
-300 -200 -100 0 100 200 300Field (kA/m)
0
100
200
300
400
Dot
s re
vers
ed
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 25
MFM Artefacts 22,22(2)
Correct domain image
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 26
MFM Artefacts 24,24(2)
Correct bit pattern
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 27
MFM Artefacts 26,26(2)
Interference stripes
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 28
MFM Artefacts 28,28(2)
Topographic contrast
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 29
MFM Artefacts 30,30(2)
Topographic contrast 2
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 30
MFM Artefacts 31,31(1)
Interaction
• Sample disturbs tip
• Tip disturbs sample
• Reversible/Irreversible
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 31
MFM Artefacts 33,33(2)
Tip reversal on strong sample
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 32
MFM Artefacts 35,35(2)
Tip reversal in external field
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 33
MFM Artefacts 37,37(2)
Domain in tip
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 34
MFM Artefacts 39,39(2)
Sample disturbance
• Reversible (susceptibility contrast)
• Irreversible
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 35
MFM Artefacts 41,41(2)
Susceptibility contrast
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 36
MFM Artefacts 43,43(2)
Move domain walls
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 37
MFM Artefacts 45,45(2)
Disturb sample
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 38
MFM Artefacts 47,47(2)
Dot switch
Data StorageLeon Abelmann Constanta Summerschool, Sep 2005 Slide 39
Conclusions 49,49(2)
Conclusions
• Imaging principle (deflection, phase, frequency)
• Fourier transform for image formation
• Side coated tips
• Noise, bandwidth
• Artefacts (interference, topography)
• Tip/sample interaction
Leon Abelmann Constanta Summerschool, Sep 2005 Slide 40