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Atomic-sized Conductors: Chains of Atoms and Hydrogen Molecules
Jan van RuitenbeekKamerlingh Onnes Laboratorium
2
What will be discussed
1. Chains of metal atoms
MD simulation Au, 12 K. Sørensenet al., PRB 57, 3283 (1998)
3
What will be discussed2. Conductance of a single hydrogen molecule
R.H.M. Smit et al. Nature, in print.
4
In collaboration with ...Leiden: Helko van den Brom, Martijn Krans, Bas Ludoph,
Chris Muller, Yves Noat, Niko van der Post, Roel Smit, Carlos Untiedt, Alex Yanson.Marc van Hemert
IBM Yorktown Heights: Norton LangMadrid: Nicolas Agraït, Gabino Rubio, Juan-Carlos Cuevas,
Alfredo Levy Yeyati, Alvaro Martin-RoderoSaclay: Michel Devoret, Daniel Esteve, Cristian UrbinaKonstanz: Elke Scheer
5
Mechanically Controllable Break Junction
6
0 50 100 150 200 250 300012345678
Gold, 4.2 KC
ondu
ctan
ce (2
e2 /h)
Piezo-voltage (V)
7
Quantum conductance (2 dimensions)
Incoming and reflected modes
Scattering at the contact
Transmitted modes
8
Conductance is transmission
Vector of incoming waves from the left, on a basis of quantum modes:
Vector of outgoing waves to the right, on a basis of quantum modes:
Matrix of transmission amplitudes:
Landauer:
lir
ror
lr itorr ˆ=
∑==n
nThett
heG
22 2)ˆˆTr(2 √
9
0 1 2 3 4 50
2
4
Aluminium, T=100 mKeI
/G∆
eV/∆
1 20
2
4
Scheer et al., PRL 78, 3535 (1997)
Superconducting subgap structure
10
Fitting procedure: demonstration
11
1 2 3 40.0
0.1
0.2
0.3
5%
20%10%
x=0%
Exce
ss n
oise
(2eI
)
Conductance (2e2/h)
Gold, 4.2 K
van den Brom & JvR, PRL 82 (1999) 1526
Shot noise
12
0 1 20.00.10.20.30.40.50.60.70.80.91.0
N=3N=2
Gold
Aluminium
Exce
ss n
oise
(2eI
)
Conductance (2e2/h)
13
Conductance fluctuations: 3 examples
-50 0 501.58
1.60
1.62
1.64
1.66
1.68
1.70
G (V
) = d
I/dV
(2e2 /h
)
-50 0 50
0.99
1.01
1.03
1.05
1.07
1.09
Bias voltage (mV)-50 0 50
0.82
0.84
0.86
0.88
0.90
0.92
0.94
Au
14
Principle of conductance fluctuationsin ballistic contacts
DiffusiveBank
DiffusiveBankBallistic
PointContact
ttar'rat
rtat'
γ
15
RMS fluctuations measured for Au
Au
0 1 2 3 40.00.20.40.60.81.01.21.41.61.82.0
G [2e2/h]
σG
V [G
o/V]
Gold
16
The modes determined by valence orbitals
Element Type ofatom
Number ofmodes
Conductance forone atom
Au s 1 1 G0
Al s-p 3 ~0.8-1.2 G
Pb s-p 3 ~2.5-3 G
Nb s-d 5 ~2.5-3 G
Cuevas et al., PRL 80 (1998) 1066
17
Chains of single atoms
18
Conductance curves for gold contacts at 4.2 K
0 4 8 12 16 20 24 28 320
1
2
3
4
5
6
7
8
Plateau length
Return distance
Con
duct
ance
(2e2/h
)
Electrode displacement (Å)
0 4 8 12 16 20
5
10
15
20
25
Ret
urn
dist
ance
(Å)
Plateau length (Å)
19
Histogram of lengths of last plateau, Au 4.2 K
0 2 4 6 8 10 12 14 16 18 20 220
50
100
150
200
x10
Num
ber o
f tim
es e
ach
leng
th is
obs
erve
d
Length of the last plateau (Å)
14 16 18 20 22
Yanson et al., Nature 395 (1998) 783
2.5 ± 0.2 Å
20
Combined TEM and STM
3.5—4 Å
Ohnishi, Kondo and Takayanagi Nature 395, 780 (1998)
21
Surface reconstructions
A
B
b)
a) [001]
[10]1
(100) surface (110) surface
22-5 -4 -3 -2 -1 0 1
0
5
10
15
20
[2e2 /h
]
Con
duct
ance
Piezo Voltage [V]
-1.0 -0.5 0.0 0.5 1.0 1.5
Pt
Electrode Displacement [nm]
0 1 2 3 4 5 6 7 8 9 100
1
2
3
4
5
Pt
Nor
mal
ised
cou
nts
[a.u
.]Conductance [2e2/h]
stop
stop
start
start
23
Test of chain formation for other metals
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.40
10
20
30
Nor
mal
ized
num
ber o
f cou
nts
[a.u
.]
Plateau length [nm]
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.402468
1012
Pd
Pt
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
Au / AgIr / Rh
4d
5d
Pt / Pd
fract
ion
of lo
ng p
late
aus
Smit et al., PRL 87, 266102 (2001)Bahn and Jacobsen, ibid., 266101
24
Relativistic effects in the bonding of Au
-0.5 0.0 0.5 1.00
1
2
3
D
ensi
ty o
f sta
tes
(arb
. un.
)
Energy
EF
25
Relativistic effects in the bonding of Au
-0.5 0.0 0.5 1.00
1
2
3
D
ensi
ty o
f sta
tes
(arb
. un.
)
Energy
EFBohr radius
2
0 2
02
4
1 ( / )
aZme
mmv c
π ε0=
=−
h
N. Takeuchi et al., PRL 63, 1273 (1991)
26
Chain formation in transition metals
Fe Co Ni Cu Zn
Ru Rh Pd Ag Cd
Os Ir Pt Au Hg
Smit et al., PRL 87, 266102 (2001)Bahn and Jacobsen, ibid., 266101
27
Conductance of a single hydrogen molecule
28
Conductance curve for Pt/H2
0.0 2.0 4.0 6.00
1
2
3
4
5
Pt/H2
Pt
C
ondu
ctan
ce (2
e2 /h)
Piezovoltage (V)
29
0 1 2 3 4 5 6 7 80.0
0.2
0.4
0.6
0.8Pt/H2
Pt
N
umbe
r of c
ount
s
Conductance (2e2/h)
Conductance histogram for Pt/H2
Bias voltage 140 mV
30
Principle of point contact spectroscopy
Ef+eV/2
Ef-eV/2
G decreases for eV > hν
Ener
g y
31
Point contact spectrum for Pt/H2
0.92
0.93
0.94
0.95
-100 -50 0 50 100-0.05
-0.04
-0.03
-0.02
-0.01
0.00
0.01
0.02
0.03
0.04
Pt/H2
D
iffer
entia
l con
duct
ance
(2e2 /h
)
63.5 mV
- 63.5 mV
dG/d
V (a
.u.)
Bias voltage (mV)
Modulation: 1 mV, 7 kHzRecording time: 10 sTemperature: 4.2 K
Numerical results for Pt-H-H-Pt
Symm., longit.: 68 meVAsymm., longt.: 431 meV
32
Isotope shift
30 40 50 60 70 800123456789
10Pt + HD
Pt + D2
Pt + H2
Cou
nts
Vibration mode energy [meV]
35 40 45 50
40 45 50 55 60
45 50 55 60 65 70 750
1
2
3
4
5
6
7
8
9
10
Cou
nts
Vibration mode energy [meV]
Pt-H2 not scaled Pt-D2 by √2 Pt-HD by √(3/2)
33
Conductance fluctuations
0 10
1000
2000
3000
4000
5000
6000
0
1
2
3
C
ount
s
Conductance (2e2/h)
σG
V (a
.u.)
T = 0.97 (1)
34
Conclusions
Universiteit Leiden