Post on 31-Mar-2015
11 April 2023 Niels Bohr Institute – University of Copenhagen
Josephson junctions and spin-electronics with single wall carbon nanotubes
Experiment: Jeppe Holm, Henrik Ingerslev Jørgensen, Kasper Grove-Rasmussen, Jonas Hauptmann, Poul Erik LindelofTheory: Jens Paaske, Karsten Flensberg,
Niels Bohr Institute & Nano-Science CenterUniversity of Copenhagen, Denmark
Symposium on Quantum Phenomena and Devices at Low Temperatures 28.-30.3.2008, ULTI users meeting, Finland
CARDEQ(ULTRA-1D)SECOQCERA QISTFTP (DK)NTT BRL
Content11 April 2023 Niels Bohr Institute – University of Copenhagen
1. Single wall carbon nanotubes by CVD2. Nanotube synthesis in its enfancy3. Biasspectroscopy4. Importance of contact resistance5. Renormalization shifts6. Exchange fields from ferromagnetic contacts7. Spin reversal by the gatevoltage8. Giaever tunneling through SWCNT9. Josephson tunneling through SWCNT
11 April 2023 Niels Bohr Institute – University of Copenhagen
CVD growth of Single-Wall Carbon Nanotubes (SWCNT)
Argon
Hydrogen
CVD oven (850 oC) Methane
11 April 2023 Niels Bohr Institute – University of Copenhagen
Carbon nanotubesarmchair Zig-Zag Chiral
(10,10) (15,0) (12,8)
1 nm
11 April 2023 Niels Bohr Institute – University of Copenhagen
Rope of single wall carbon nanotubes
10 nm
TEM picture
11 April 2023 Niels Bohr Institute – University of Copenhagen
SWCNT with topgates and backgates
10/26/2005
Bandstructure of Carbon nanotubes
(N, M) = (5, 5) (N, M) = (10, 5)
Metallic tubes (but…) Wide-gap semiconducting tubes
Chirality determines bandstructure
11 April 2023 Niels Bohr Institute – University of Copenhagen
__ __
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source drain
Quantum dot
barriere barriere
Vgate
Vsd
Vsd
0 -
Vgate
* * * *___________
Transconductance ~ 3e2/h
Quantum DotsBias-spectroscopy
11 April 2023 Niels Bohr Institute – University of Copenhagen
Fabry-Perot/Kondo/Coulomb
K. Grove-Rasmussen et al.
J. New Physics (2006)
Coulomb blockade shells)
Adding 285 electrons,one by one...
88 odd-occupiedcharge states withzero-bias Kondo ridge.
11 April 2023 Niels Bohr Institute – University of Copenhagen
4 shell Kondo resonances
Vg
Jeppe Holm, MSc
The standard diamond
H He Li Be
B C N O
F Ne Na Mg
... ... ... ...
Shell-filling
11 April 2023 Niels Bohr Institute – University of Copenhagen
Kondo resonance
.
The standard shell diamonds
Inelastic cotunneling
Elastic cotunneling (S=½ Kondo)
New type of diamondsGatedependent excitation energies
30
21
7
53 are unidentified
11 April 2023
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Renormalization effects *** *
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_ __ _
_ _
- large transmission
- small transmission
Tunneling-renormalized diamonds (Theory)
Diamond edges are skewed
Widths of diamonds are different
11 April 2023 Niels Bohr Institute – University of Copenhagen
Relative width of the different diamonds
11 April 2023 Niels Bohr Institute – University of Copenhagen
Exchange field*
Hauptmann, Paaske, Lindelof, Nature Physics, April 2008
*Ideas of Patsupathy et al. (2004) Martinek et al. (2005)
11 April 2023 Niels Bohr Institute – University of Copenhagen
Exchange field and external
field
Hauptmann, Paaske, Lindelof, Nature Physics, April 2008
11 April 2023 Niels Bohr Institute – University of Copenhagen
Gate influence on exchange field
11 April 2023 Niels Bohr Institute – University of Copenhagen
Renormalizationllevel shift for
various Vg and B
Hauptmann, Paaske, Lindelof, Nature Physics, April 2008
Theory of Martinek et al.PRB 72, 121302 (2005)
- - - 2. Order perurbation theory
11 April 2023 Niels Bohr Institute – University of Copenhagen
-10 -5 0 5 10
-6
-3
0
3
6
Vgate [V]
Vsd
[mV]
PdNbPd-SWCNT-PdNbPd (5/70/5nm)• Gap around zero bias, width corresponding to 4• Clear Coulomb blockade diamonds
Vsd = 2
Superconducting Giaever tunnelling
Henrik I. Jørgensen, Kasper Grove-Rasmussen and PEL
11 April 2023 Niels Bohr Institute – University of Copenhagen
-3 -2 -1 0 1 2 30.00
0.05
0.10
0.15
0.20
0.25
QPQP
ES
dI/
dV
[e
2/h
]
Vsd [mV]
A B
GS
GS
GS
QP
QP
2
-2
=20uV (5nA)Ec = 5-6 meV = 0.275 meVE = 2-3 meV
Ec, E >>>>
PdNbPd-SWCNT-PdNbPd (Coulomb blockade)
Henrik I. Jørgensen, Kasper Grove-Rasmussen and PEL
S-SWCNT-S
E
11 April 2023 Niels Bohr Institute – University of Copenhagen
Designed Bias circuit to superconducting SWCNT
11 April 2023 Niels Bohr Institute – University of Copenhagen
Josephson effect & p junctions
H.I. Jørgensen et al., Nano Letters 7, 2441 (2007)
TiAlTi-SWCNT-TiAlTiTc=0.75 KD=0.1 meV
T=75 mK
11 April 2023 Niels Bohr Institute – University of Copenhagen
Ic (Vg)
H.I. Jørgensen et al., Nano Letters 7, 2441 (2007)
Summary
11 April 2023 Niels Bohr Institute – University of Copenhagen
- Fabrication of SWCNTs is still rudimentary- Contacts resistance < = < h/4e2 crucial, but it is not well
controlled (~30%)- We found a new renormalization effect in SWCNT- We measured a magnetic exchange field (~2 T) in
SWCNT with ferromagnetic contacts- We are for the first time able to reverse a single electron
spin in a quantum dot by tuning a backgate voltage- We optimized the Josephson supercurrent by a bias circuit
(up to 2.5 nA, D/eRJ=4.5 A)- We studied S-SWCNT-S p - Josephson junction