electron transport through single atoms and molecules · electron transport through single atoms...
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Electron Transport throughSingle Atoms and Molecules
J. Kröger, University of Kiel
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Acknowledgements
Experiment
N. Néel, L. Limot, R. Berndt
Theory
Th. Frederiksen, M. Brandbyge (Denmark)K. Palotas, A. Garcia-Lekue, W.A. Hofer (United Kingdom)
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Conductance
A
L
L
a
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G0 2 G0 3 G0
tip
sample
constriction: atom, cluster, molecule
x
y
z
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Conductance quantization in experiments
Van Wees et al., PRL 60, 848 (1988)
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Mechanically controlled break junctions
1 μmVan Ruitenbeek, Agraït, Scheer
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Number of conductance channels
=
Number of valence orbitals
Scheer et al., Nature 394, 154 (1998)
Cuevas et al., PRL 80, 1066 (1998)
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Tip
Sample
Ohnishi et al., Nature 395, 780 (1998)
Vacuum
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UHV, 7 K
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Tip-surface contactLimot, Kröger, Berndt, Garcia-Lekue, Hofer
PRL 94, 126102 (2005)
10-5
10-4
10-3
10-2
10-1
100
G (2
e2 /h)
-6 -5 -4 -3 -2 -1 0
Displacement (Å)
3
4
5
6
789
100
-5.3 -5.2 -5.1
∆ zc
Gc
Cu(111)
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Displacement Δz
Tunnelling Transition Contact
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Tip-adatom contact
10-5
10-4
10-3
10-2
10-1
100
G (2
e2 /h)
-5 -4 -3 -2 -1 0
Displacement (Å)
Cu(111) – Cu
Ag(111)PRL 94, 126102 (2005)
Au(111)New J. Phys. 9, 153 (2007)
3
4
5
6
7
8
9100
-5.2 -5.1 -5.0 -4.9
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Probing the conductanceof individual molecules
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1
2 3
4
Cu(100) – C60
: 4 molecule orientations
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1 42 3
LUMO + 1
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Néel, Kröger, Limot, Frederiksen, Brandbyge, Berndt, PRL 98, 065502 (2007)
tunnelling
transition
contact
1
Tip – Molecule Contact
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Fluctuations in transition regime
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Local heating
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More power – more heating
Teff
≈ 300 K
Teff
≈ 400 K
Teff
≈ 700 K
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Orientation-dependent conductance
Néel, Kröger, Limot, Berndt, Nano Letters, published online
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1 2 3 4
0.26 G0
0.25 G0
0.26 G0
0.17 G0
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Spectroscopy of molecular orbitals
HOMO
LUMO
LUMO+1
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1 2 3 4
Conductingstrongly
Conductingweakly
Overlap of orbitals
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Rotation in a single-molecule contact
Néel, Limot, Kröger, BerndtPRB 77, 125431 (2008)
SFB 677:Function by Switching
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Threshold behaviour
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Controlled contact to magnetic atoms
SFB 668: Magnetism from the single atomto the nanostructure
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Kondo effect of magnetic impurities
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tunnelling
contact
Broadening of Kondo resonance
Néel, Kröger, Limot, Berndt, Palotas, Hofer, PRL 98, 016801 (2007)
Cu(100) – Co
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350
300
250
200
150
100
50
T K (K
)
-6 -5 -4 -3 -2 -1 0∆ z (Å)
Increase of Kondo temperature
tunnelling
contact
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-4
-2
0
2
4D
ensi
ty o
f sta
tes
(1/e
V)
-4 -3 -2 -1 0 1 2E - EF (eV)
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Spin-integrated transport
Spin-polarized transport
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Cobalt islands on Cu(111)
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Electron transport through single magnetic atom
Cu(111)
Co atom
Co island
Electrode combinations:
Cu – Co – Cu Cu – Co – Co Ni – Co – Co
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Cu – Co – Cu:
Cu – Co – Co:Ni – Co – Cu: ≈ 0.8 G
0
Ni – Co – Co: ≈ 0.5 G0
≈ 1.0 G0
Néel, Kröger, Berndt, Brandbyge, in preparation
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Summary
Kröger, Néel, Limot, J. Phys.: Condens. Matter, at press
Outlook• Extension to other molecules
• Time-resolved fluctuations
• Vibration spectroscopy
• Spin-polarized transport