magnetism at the atomic scale by scanning probe techniques · → sp-stm is advanced in periodic...
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University of Hamburg K. von Bergmann
Magnetism at the atomic scale Magnetism at the atomic scale by Scanning Probe Techniques by Scanning Probe Techniques
Kirsten von BergmannKirsten von Bergmann
Institute of Institute of AppliedApplied PhysicsPhysicsUniversityUniversity ofof HamburgHamburg
University of Hamburg K. von Bergmann
Magnetism with SPMMagnetism with SPM
Spin-polarized scanning tunneling microscopy SP-STM→ density of states of a magnetic sample is spin-polarized(now used in various groups worldwide)
Spin-flip excitation spectroscopy with STM→ excitation of allowed transition adds an inelastic contribution(group of Andreas Heinrich, IBM Almaden)
Magnetic exchange force microscopy MExFM→ direct exchange interaction between probe tip and sample(U. Kaiser, A. Schwarz, R. Wiesendanger, Univ. Hamburg)
University of Hamburg K. von Bergmann
Scanning tunneling microscopyScanning tunneling microscopy
),()(d
dst eUETeU
U
I⋅⋅∝ ρρ st ⋅⋅∝ ρρ st ⋅⋅∝ ⋅⋅∝ ),()( ),()( ),()( ),()( ),()(
LDOS
local densityof states
φt
φs
tip sample
2
sample
U
I
tip
ddEeUETEeUEI
eU
⋅⋅∝0
st ),()(),( ρρ
topography:topography:
constantconstant--current modecurrent mode
scan
tip
sample
d dI/dU spectrum at point x,y
ddII/d/dUU spectroscopyspectroscopy
University of Hamburg K. von Bergmann
spinspin--polarized LDOSpolarized LDOS
spin-imbalance atthe Fermi-energy
spin-polarized current
magnetic material
University of Hamburg K. von Bergmann M. Bode, Rep. Prog. Phys. 66, 523 (2003).
spinspin--polarizedpolarized STMSTM
spinspin conservationconservationduringduring thethe
tunneltunnel processprocess
M. Julliere, Phys. Lett. 54A, 225 (1975).
mag
n. t
ipm
agn.
tip
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angularangular dependencedependence
J. C. Slonczewski,Phys. Rev. B 39, 6995 (1989).
T. Miyazaki and N. Tezuka,J. Magn. Magn. Mater. 139, L231 (1995).
spin-averaged
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magnetic tip material
thin film coating FM and AFM
optically pumped GaAs tips
spinspin--polarized probepolarized probe
FM AFM
→ reduction of stray field→ control over direction of magnetization
University of Hamburg K. von Bergmann
thinthin film tipsfilm tips
flashedflashed tiptip hashas radiusradius ~ 500 nm~ 500 nm→→ surfacesurface andand interfaceinterface
anisotropyanisotropy dominatedominate→→ MM dependsdepends onon thinthin film materialfilm material
M. Bode et al., Phys. Rev. Lett. 81, 4256 (1998)M. Bode, Rep. Prog. Phys. 66, 523 (2003).
2µm
FeFe--coatedcoated WW tiptipsensitive to sensitive to inin--planeplanemagnetizationmagnetization componentcomponent
CrCr--coatedcoated WW tiptipsensitive to sensitive to outout--ofof--planeplanemagnetizationmagnetization componentcomponent
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modulation techniquemodulation technique
W. Wulfhekel and J. Kirschner,Appl. Phys. Lett. 75, 1944 (1999).
U. Schlickum, W. Wulfhekel, and J. Kirschner,Appl. Phys. Lett. 83, 2016 (2003).
FM tip material
sensitive to out-of-plane… … or in-plane magnetization
University of Hamburg K. von Bergmann
thin film tips vs modulation technique thin film tips vs modulation technique
U. Schlickum, W. Wulfhekel, and J. Kirschner,Appl. Phys. Lett. 83, 2016 (2003).
separation oftopography and magnetic signal
thin film tips
modulation technique
measurement of I(U)and dI/dU(U)
contains informationon structural,electronic and
magnetic properties
M. Bode, Rep. Prog. Phys. 66, 523 (2003).
University of Hamburg K. von Bergmann
SPSP--STM:STM: spectroscopyspectroscopy modemode
e.ge.g. 1.3 AL Fe on W(001). 1.3 AL Fe on W(001)2nd ML 2nd ML isis ferromagneticferromagnetic→→ 44 magneticmagnetic domainsdomains
sideside viewview
“spin-averaged“
University of Hamburg K. von Bergmann
SPSP--STM:STM: spectroscopyspectroscopy modemode
spin-resolved
e.ge.g. 1.3 AL Fe on W(001). 1.3 AL Fe on W(001)2nd ML 2nd ML isis ferromagneticferromagnetic→→ 44 magneticmagnetic domainsdomains
inin--planeplane sensitivesensitive magneticmagnetic tiptip
sideside viewview
K. von Bergmann et al.,Phys. Rev. B. 70, 174455 (2004).
University of Hamburg K. von Bergmann
SPSP--STM:STM: spectroscopyspectroscopy modemode
e.ge.g. 1.3 AL Fe on W(001). 1.3 AL Fe on W(001)2nd ML 2nd ML isis ferromagneticferromagnetic→→ 44 magneticmagnetic domainsdomains
inin--planeplane sensitivesensitive magneticmagnetic tiptipddII//ddUU mappingmapping atat UU=+50mV=+50mV
toptop viewviewMtip
University of Hamburg K. von Bergmann
SPSP--STM:STM: constantconstant--currentcurrent modemode
e.ge.g. 1.3 AL Fe on W(001). 1.3 AL Fe on W(001)1st1st ML ML isis outout--ofof--planeplane AFMAFM→→ atomicatomic scalescale magnetismmagnetism
c(2c(2××2) AFM2) AFM
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c(2c(2××2) AFM2) AFM
SPSP--STM:STM: constantconstant--currentcurrent modemode
Mtip
S. Heinze et al., Science 288, 1805 (2000).D. Wortmann et al., Phys. Rev. Lett. 86, 4132 (2001).S. Heinze, Appl. Phys. A 85, 407 (2006).
2 nm
[100][100]
topographytopography
A. Kubetzka et al.,Phys. Rev. Lett. 94, 087204 (2005).
University of Hamburg K. von Bergmann
investigating single magnetic atomsinvestigating single magnetic atoms
F. Meier, L. Zhou, J. Wiebe, and R. Wiesendanger,Science 320, 82 (2008).
Co atoms on Pt(111)
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magnetization curves of individual atomsmagnetization curves of individual atoms
Cr-
tip
+Bext
Cr-
tip
+Bext
F. Meier, L. Zhou, J. Wiebe, and R. Wiesendanger,Science 320, 82 (2008).
University of Hamburg K. von Bergmann
Magnetism with SPMMagnetism with SPM
Spin-polarized scanning tunneling microscopy SP-STM→ density of states of a magnetic sample is spin-polarized(now used in various groups worldwide)
Spin-flip excitation spectroscopy with STM→ excitation of allowed transition adds an inelastic contribution(group of Andreas Heinrich, IBM Almaden)
Magnetic exchange force microscopy MExFM→ direct exchange interaction between probe tip and sample(U. Kaiser, A. Schwarz, R. Wiesendanger, Univ. Hamburg)
University of Hamburg K. von Bergmann
A.J. Heinrich, J.A. Gupta, C.P. Lutz, and D.M. Eigler,Science 306, 466 (2004).
University of Hamburg K. von Bergmann
spinspin--flip excitation spectroscopyflip excitation spectroscopy
C.F. Hirjibehedin, C.P. Lutz, and A.J. Heinrich,Science 312, 1021 (2006).
C.F. Hirjibehedin, C.-Y. Lin, A.F. Otte, M. Ternes, C.P. Lutz, B.A. Jones, and A.J. Heinrich,Science 317, 1199 (2007).
coupling between magnetic atomsanisotropy of magnetic atoms
University of Hamburg K. von Bergmann
Magnetism with SPMMagnetism with SPM
Spin-polarized scanning tunneling microscopy SP-STM→ density of states of a magnetic sample is spin-polarized(now used in various groups worldwide)
Spin-flip excitation spectroscopy with STM→ excitation of allowed transition adds an inelastic contribution(group of Andreas Heinrich, IBM Almaden)
Magnetic exchange force microscopy MExFM→ direct exchange interaction between probe tip and sample(U. Kaiser, A. Schwarz, R. Wiesendanger, Univ. Hamburg)
University of Hamburg K. von Bergmann
magnetic exchange force microscopymagnetic exchange force microscopy
NiO: antiferromagnetic dueNiO: antiferromagnetic due
to superexchange betweento superexchange between
Ni atoms via O bridgesNi atoms via O bridges
bulk terminated surface magnetic structure bulk terminated surface magnetic structure →→ canted spin canted spin
concept of MExFM
detecting the direct magnetic
exchange interaction
short-range force between
the last magnetic tip atom and
the magnetic atomon the sample
U. Kaiser, A. Schwarz, and R. Wiesendanger, Nature 446, 522 (2007).
University of Hamburg K. von Bergmann
magnetic exchange force microscopymagnetic exchange force microscopy
chemical contrast:Ni - O = 4.5 pm
MExFM contrast:Ni↑-Ni↓ = 1.5 pm~30 pm closer
U. Kaiser, A. Schwarz, and R. Wiesendanger, Nature 446, 522 (2007).
University of Hamburg K. von Bergmann
summarysummary
→ SP-STM is advanced in periodic structures andis reaching for small structures and atoms
→ Spin-flip excitation spectroscopyexplores the quantum magnetic behavior
of small structures and atoms
→ MExFM is the choice for insulating samples