on the subtle interplay of light induced magnetization, driven currents and … · 2018. 11. 6. ·...
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Delay
… study by the seaside
@spintronicsHGW
On the subtle interplay of light induced
magnetization, driven currents and heat in
ultrafast magnetism… ways towards optical spin manipulation in topological systems
Markus Münzenberg
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THz spintronics and ultrafast magnetism
Perspective, J. Appl. Phys. 120, 140901 (2016)
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Ke
rr r
ota
tio
n (
a.u
.)
Time (ps)
-5 0 5 10 15
3 ps
Out of planeCurrent bunch I
+M
-M
+M
Ultrafast trigger
Free THz B-field trigger
• Stanford accelerator
Ch. Back et al., Science (1999)
• Photoconductive switch, 1ps
rise time, 0.2 Tesla
Wang et al. JAP (2008)
• Free THz pulse (organic
crystals)
0.5 ps rise time, ~1Tesla
C. Hauri et al. Nature
Photon.(2013)
Perspective, J. Appl. Phys. 120, 140901 (2016)
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Skyrmions
Topological matter
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Internal spin-orbit field
Large spin-orbit coupling leads
to cyclotron orbit
Topological Insulators
Cyclotron resonance, in 2D
materials quantum Hall effect and
edge states
lsE so
~
h
enH
2
Topological matter
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Topological matter
From A. Fert, V. Cros, and J. Sampaio, Nat.
Nano. 8, 152–156 (2013)
Nature Phys. 5 (2009) 438-42
Phys. Rev B 82 (2010) 045122
x
y
Real space x, y Reciprocal space kx, ky
Skyrmions Topological insulators
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• The nature of femtosecond spin dynamics
• THz spintronic emitter
• Hard disc: state of the art
• Thermal model of ultrafast demagnetization
• FePt optical writing a storage media
• Summary
Outline
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Tim
e (
~1
0 fs)
Ultrafast: spins
~group velocity
Length (~nm)Perspective, J. Appl. Phys. 120, 140901 (2016)
nanoscale spin currents
charge currents je: e-
spin currents js : ms
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Tim
e (
~1
0 fs)
Ultrafast: spins
~group velocity
Length (~nm)Perspective, J. Appl. Phys. 120, 140901 (2016)
- +js
s
+ -e-
je
Nanoscale spin currents js: ms
Nanoscale charge currents je: e-
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• The nature of femtosecond spin dynamics
• THz spintronic emitter
• Hard disc: state of the art
• Thermal model of ultrafast demagnetization
• FePt optical writing a storage media
• Summary
Outline
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• Fritz-Haber Institut, Berlin, Germany
• Physics and Astronomy, Uppsala
University, Sweden
Tobias Kampfrath
Peter Oppeneer
THz: T. Kampfrath
Spintronic THz emitter
Published in Nature Nanotech. 8, 256 (2013),
Nature Photonics 10, 483–488 (2016).
Theory Spin Currents: Battiato, OppeneerTom Seifert
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• Johannes Gutenberg-Universität Mainz
• FZ Jülich
Spintronic THz emitter
Published in Nature Nanotech. 8, 256 (2013),
Nature Photonics 10, 483–488 (2016).
Mathias Kläui
Emitter: Kläui, Münzenberg
Theory SHE: Mokrousov, Freimuth
Yuri Mokrousov
Frank Freimuth
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fs pump
pulse
Pump pulse excites and electrons
: d sp bands become fast
Oppeneer et al., PRL (2010)
Fe (~5 nm)
Spintronic THz emitter
Ferromagnet
Nature Nanotech. 8, 256 (2013).
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Inverse spin Hall effect (ISHE):
Spin-orbit coupling deflects electrons
transverse charge current
Spin hall angle
fs pump
pulse
Metal (NM)
Fe (~5 nm)
g
Spintronic THz emitter
Kampfrath, Battiato, Oppeneer, Wolf,
Freimuth, Mokrousov, Münzenberg et al.,
Nature Nanotech. 8, 256 (2013)
𝛾 =𝜎SH𝜎𝑥𝑥
𝜎SH - spin Hall
conductivity
𝜎𝑥𝑥 - diagonal
conductivityjc
g
js
Ferromagnet
Nature Nanotech. 8, 256 (2013).
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Measure THz emission from photoexcited FM/NM bilayers
Kampfrath, Battiato, Oppeneer, Wolf,
Freimuth, Mokrousov, Münzenberg et al.,
Nature Nanotech. 8, 256 (2013)
Note: just used a pulsed
laser oscillator (10 fs, 80 MHz)
Spintronic THz emitter
fs pump
pulse
MetalFe (~5 nm)
g
300µm GaP,
10fs gate pulse
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TH
z s
ign
al
(10
-5)
t (ps)
+M
-M
0 0.5 1-3
-2
-1
0
1
2
3
FePt
Transient changes polarity by reversing M or stacking order
Fe Pt
TH
z s
ign
al
(10
-5)
t (ps)0 0.5 1
-3
-2
-1
0
1
2
3
Really SHE scenario? change NM layer
Spintronic THz emitter
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Calculations:
Freimuth, Blügel,
Mokrousov
e.g. PRL (2010)
Good relative agreement
Simple method to get relative estimates of spin-Hall conductivity
4
3
2
1
0
-1
-2
NM material
1
0.8
0.6
0.4
0.2
0
-0.2
-0.4
Cr Pd Ta W Ir PtPt38Mn62
TH
zam
plit
ude
(norm
aliz
ed
)
Ca
lc. s
pin
Hall c
onductiv
ity(1
05
S m
-1)
Co
Fe
B
NM
Is CoFeB/Pt useful as a THz emitter?
Spintronic THz emitter
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180
160
140
120
100
80
60
40
20
0
-20
Ele
ctr
ic f
ield
(V
/cm
)
3210
t (ps)
STE
ZnTe (1mm)
PCS
3
4
5
6
7
89
0.1
2
3
4
5
6
7
89
1
|Ele
ctr
ic f
ield
| (a
rb. u
nits)
302520151050
/ 2(THz)
Spintronic metalic emitter outperforms standard emitters over large frequency intervals
Spintronic THz emitter
(5.8 nm)
(interdigitated, SI-GaAs)
Comparison to standard emitters: Spintronic Emitter (STE),
Photoconductive Switch (PCS)
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20fs,
0.3mJ300µm GaP,
10fs gate pulse
Bi2Se3
Bi2Se3+
-
• THz emission is
polarization dependent
• Circular photogalvanic
effects?
Helicity
Topological matter
• Spin-momentum locking
J. W. McIver, et al. Nature Nano.(2011).
Ganichev et al. Nature (2002).
T. Seifert and et al. (2016).
-k
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TIy
x
F
What is the source?
• Use F dependence
to reduce data
(crystal symmetry)
• THz emission Dependence of pump polarization and sample
orientation:
JS: strongly dependent on both
JP: independent
Topological matter
L. Braun, G. Mussler, et al., Nature Comm. 7, 13259
(2016).
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Topological matter
• Circular photogalvanic effect C, thermovoltage D
0 90 180 270 360
0.10
0.12
0.14 data fit
qwp angle (°)
• 3D topological insulator intrinsic doping, 16 nm
(Bi0.57Sb0.43)2Te3)
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Topological matter
• 3D topological insulator intrinsic doping, 16 nm
(Bi0.57Sb0.43)2Te3)
0 50 100 150 200 250
0
50
100
150
200
250V
ert
ica
l d
ista
nce
(
m)
Horizontal distance (m)
-1.5 0.0 1.5
D (mV)
photoV
-0.5 0.0 0.5
D (mV)
-0.3
0.0
0.3
D (
mV
)
• Circular photogalvanic effect C, thermovoltage D
𝛻T
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Topological matter
• Spin accumulation by Spin-Nernst effect
• Circular photogalvanic effect C, thermovoltage D
Detail: Hall bar
See also S. Meyer et al. Nature Materials (2017).
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• The nature of femtosecond spin dynamics
• THz spintronic emitter
• Hard disc: state of the art
• Thermal model of ultrafast demagnetization
• FePt optical writing a storage media
• Summary
Outline
![Page 25: On the subtle interplay of light induced magnetization, driven currents and … · 2018. 11. 6. · Time (ps) - 50 5 10 1 3 ps Out of plane Current bunch I +M-M +M Ultrafast trigger](https://reader035.vdocument.in/reader035/viewer/2022070207/60f842b384d46037843a85e6/html5/thumbnails/25.jpg)
• CSIC, Madrid
Oksana Chubykalo-Fesenko
Thermal macrospin modelling
Pablo Nieves, Oksana Chubykalo-Fesenko
• Western Digital Corporation, San Jose
Simone Pisana, Tiffany Santos
Tiffany Santos
FePt storage media
FePt optical writing a storage media
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• Kiel UniversityJeffrey
McCordMO-Imaging
Cai Müller, Jeffrey McCord,
• Uppsala University
Marco Berritta, Ritwik Mondal, Peter Oppeneer
• Konstanz University
Denise Hinzke, Ulrich Nowak
Uli Nowak
Inverse Faraday
FePt optical writing a storage media
Peter
Oppeneer
Thermal spin modelling
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Spin
Nanostrukturen
Interior of a hard disc
• Hard disc at fs speed
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FePt + segregant (12nm)
MgO/heat sink/adhesion layer//glass
Carbon overcoat (6nm)
Western Digital Corporation HAMR media, HC= 4T at room temperature
Hard disc at ultrafast speed
FePt-L10
+ segregant(high temp.)
heat sink
MgO seed
heat sink seed
and adhesion
20 nm
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FePt optical writing a storage media
σ-
σ+
12.7 mJ/cm2 (10 mW)
Writing using the helicity of light:
Magneto-optical contrast (Kerr microscopy)
FePt (AgCu) granular recording media
R. John, P. M. Oppeneer, U. Nowak, and M. Münzenberg, Sci. Rep. 7, 4114 (2017)
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10 20 30 40
20.0k
40.0k
60.0k
80.0k
Co
ntr
ast
(arb
itra
ry u
nit)
Position X (m)
L
-
Starting with remnant magnetization 0% Ms after
growth:
FePt optical writing a storage media
+Ms
-Ms
+
σ-l
σ +
σ -
L
σ-
X
7.5 mW (6.6 mJ/cm2 per pulse)
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FePt optical writing a storage media
+Ms
-Ms
+
σ-l
10 20 30 40-4.0k
-3.0k
-2.0k
-1.0k
0.0
1.0k
2.0k
3.0k
4.0k
Co
ntr
ast (a
rbitra
ry u
nit)
Position X (m)
L
-
10 20 30 40-4.0k
-2.0k
0.0
2.0k
4.0k
6.0k
8.0k
10.0k
12.0k
14.0k
Position X (m)
Contr
ast (a
rbitra
ry u
nit)
L
-
Demagnetized
100
Saturated
75
50
No full writing! What is the mechanism? 15 mW (13.2 mJ/cm2 per pulse)
Starting with magnetization 100% Ms, saturated case:
pu
(%)
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FePt optical writing a storage media
σ- σ+
Carbon overcoat (3nm)
MgO/NiTa/glass AgC-segregant
• Model to describe the data:
Transition rates
Laser writing region
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FePt optical writing a storage media
σ- σ+
0 5 10 15 20 25
0.0
0.2
0.4
0.6
0.8
1.0
0.0
0.2
0.4
0.6
0.8
1.0
Only MCD, no IFE
Pro
babili
ty P
u
Number of pulses
Both MCD and IFE
Starting configuration, i=0:
random
all up
all down
• Model to describe the data:
Transition rates
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• FePt (AgCu) granular recording media:
single/ multiple pulse writing
FePt optical writing a storage media
σ- σ+
5 mW (30 mJ/cm2 per pulse)
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FePt optical writing a storage media
l=800 nm
1 2 3 4 5
-0.06
-0.04
-0.02
0.00
0.02
-
KIF
E (
1/T
)
Photon energy (eV)
0 1 2 3 4 5
6
12
18
Imagin
ary
part
n
Photon energy (eV)
-
+M -M
l=800 nm
-I+I
Magnetic circular dichroism (MCD)
• What about the wave lenght dependence?
Inverse Faraday effect (IFE)
1200 nm to 1350 nm, 1.03 to 0.92 eV
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1200 nm
1250 nm
1300 nm
1350 nm 39
µm
+ -
0 100 200 300 400 500-3000
-2000
-1000
0
1000
2000
3000
Contr
ast (a
. u.)
A
0 100 200 300 400 500-3000
-2000
-1000
0
1000
2000
3000
Contr
ast (a
. u.)
A
0 100 200 300 400 500-3000
-2000
-1000
0
1000
2000
3000
Contr
ast (a
. u.)
A
0 100 200 300 400 500
-2000
-1000
0
1000
2000
3000
Co
ntr
ast
(a.
u.)
Width (m)
0 50 100 150 200
-0.0006
-0.0004
-0.0002
0.0000
Derivative Y1
0.000000 (2.000000)
1st derivative of "NaN"
Gauss Fit of C"Derivative Y1"
0 100 200
-0.0008
-0.0006
-0.0004
-0.0002
0.0000
Derivative Y1
A
1st derivative of B
Gauss Fit of C"Derivative Y1"
0 100 200
-0.0004
-0.0002
0.0000
Derivative Y1
A
1st derivative of B
Gauss Fit of C"Derivative Y1"
Gaussian laser
profiles
19 µm
20 µm
19.5 µm
18 µm
FePt optical writing a storage media
• What about the wave lenght dependence?
Writing efficiency can be increased by a factor of two to three.
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Glassy vortex networks
• What about topological objects?
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• Göttingen University
Claus Ropers
UTEM developement
Tim Eggebrecht, Marcel Möller,
Nara Rubiano da Silva, Claus
Ropers, Sascha Schäfer
Sascha Schäfer
Glassy vortex networks
T. Eggebrecht, et al., Phys. Rev. Lett. 118,
097203 (2017).
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Ultrafast Transmission Electron
Microscopy
Imaging / Diffraction /
Spectroscopy
UTEM
e-pulse
(probe)
excitation pulse
(pump)
photoemission
laser
sample
Principle
• photoemission from needle shaped
emitter
• Laser-pump/electron-probe experiments
Temporal/spatial/spectral electron pulse properties
3.3nm
2.6nm
-500 0 500
Delay (fs)
300f
s
-2 -1 0 1 2
Energy (eV)
0.6 eV
Glassy vortex networks
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Lorentz imaging with ultrashort electron pulses
2 µm
Imaging conditions
• 1.5 e-/pulse
• 250 kHz rep.
rate, 60 s
exposure
• Total electron
number: 2x107 e-
Δf < 0
Out-of-focus(add. magnetic
contrast)
• permalloy thin
film on silicon-
nitride membrane
• FIB patterned
magentic nano
islands
Magnetic vortex
structure
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Writing of vortex networks
Network
Magneti
-zation
Electron
intensity
Phase
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Writing of vortex networks
Well defined network that depends on the quench rate
T. Eggebrecht, et al.,
Phys. Rev. Lett., 2017.
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Writing of vortex networks
Well defined network that depends on the quench rate
T. Eggebrecht, et al.,
Phys. Rev. Lett., 2017.
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• Kiel UniversityJeffrey
McCordMO-Imaging
Enno Lage, Jeffrey McCord,
• Konstanz University
Ulrich Nowak
Uli Nowak
Skyrmion-Bubbles
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1 mm
5 m5 m5 m
Field conditioning Single skyrmions Dense skyrmions
Writing of vortex networks
• Skyrmions with diameters below 200 nm, DMI
Ta/CoFeB/MgO layer wedge system
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• Tilted magnetic field
• In plane static magnetic field with
1° tilt
• Bubbles grow with decreasing field
• Zero field stable bubble phase
dCoFeB = 1.367 nm to 1.375 nm
1.36 1.37 1.380
2
4
stable
ip nucleation
+
oop nucleation
stable
ip nucleation
instable
0H
Z (
mT
)
CoFeB thickness (nm)
instable
Writing of vortex networks
100 mT @ 1° 70 mT @ 1° 35 mT @ 1° 12 mT @ 1° 0 mT @ 1°
5 m
Increasing Htilted
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40 µm
0 s
6 s
4 s
2 s
Forward
+ -
38V at 545Ohm => I = 2 e12 A/m^2 (2e8 A/cm^2)
B = 0,56 mT
• Forward and
backward motion
• Currents needed
j=2 108 A/cm2
• Already in
regime of current
induced bubble
generation by
heat pulses
Show vid_probe2_8.avi
38V at 545Ohm => I = 2 e12 A/m^2 (2e8 A/cm^2)
B = 0,69 mT
Backwards
198 s
132 s
66 s
0 s
+-
Writing of vortex networks
• Current driven motion: 10 µm constriction
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• Current driven motion: 10 µm constriction
Writing of vortex networks
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• Current driven motion: 10 µm constriction
Writing of vortex networks
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0 5 10 15-20
-15
-10
-5
0
x (
µm
)
t (s)
0 5 10 15
-2
-1
0
1
2
y (
µm
)
t (s)
0 5 10 15-20
-15
-10
-5
0
x (
µm
)
t (s)
0 5 10 15
-2
-1
0
1
2
y (
µm
)
t (s)
0 5 10 15-20
-15
-10
-5
0
x (
µm
)
t (s)
0 5 10 15
-2
-1
0
1
2
y (
µm
)t (s)
Skyrmion 1 Skyrmion 2 Skyrmion 3
Writing of vortex networks
• Motion tracking – testing the local potential
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• Motion tracking
SPP Skyrmionics
Writing of vortex networks
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• The nature of femtosecond spin dynamics
• THz spintronic emitter
• Hard disc: state of the art
• Thermal model of ultrafast demagnetization
• FePt optical writing a storage media
• Writing of topological objects
• Summary
Outline
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Contributions
Priority program
SpinCaT
Priority program
Topologische Isolatoren
Magnonics: Materials and
Devices
Robin JohnJakob Walowski
@spintronicsHGW
Ulrike Martens
Christian Denker
Priority program
Skyrmionics
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Collaborations
J. Nötzold, S. Mährlein, Lukas Braun, Tobias
Kampfrath, Fritz Haber Institute
C. Franz, C. Heiliger, Gießen University
Gregor Mussler, Detlev Grützmacher, FZ
Jülich
F. Katmis, J. S. Moodera, MIT Cambridge
Pablo Nieves, Oksana Chubykalo-Fesenko,
CSIC, Madrid
J. McCord, C. Müller, Kiel University
A. Thomas, IFW Dresden
Sascha Schäfer, Oldenburg University
Claus Ropers, Göttingen University
Tiffany Santos,
Western Digital Cooperation San Jose
Uli Nowak, Denise Hinzke, Konstanz University
Mathias Kläui, Mainz University
Ilie Radu, Max-Born-Institute, Berlin
Marco Battiato, Pablo Maldonado, Peter
Oppeneer, Uppsala University
F. Freimuth, Y. Mokrousov, S. Blügel, FZ Jülich
Dagmar Butkovicova, Eva Schmoranzerová,
Charles University Prague
Günter Reiss, Thorsten Hübner Timo Kuschel
Bielefeld University
@spintronicsHGW
SPP Skyrmionics
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Greifswald
See NDR feature on our new labs: Nordmagazin or http://www.physik.uni-greifswald.de/
aktuelles.html @spintronicsHGW
Physics