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Kondo Effects in Carbon Nanotubes Master Colloquium by Jeppe Vilstrup Holm Supervisor: Poul Erik Lindelof

Kondo Effects in Carbon Nanotubes Master Colloquium by Jeppe Vilstrup Holm Supervisor: Poul Erik Lindelof

Outline

Single wall carbon nanotubes (SWCNT) Quantization effects SWCNT quantum dots The Kondo effect in bulk Kondo effects in carbon nanotubes Equilibrium In equilibrium Conclusion

Outline

Single wall carbon nanotubes (SWCNT)

Single Wall Carbon Nanotubes

a2 a1 Carbon atom Graphene ~1 nm

One dimensional conductor. Metallic or Semiconducting

Metallic Semiconducting Metallic Metallic if: 2n+m/3=q

Outline

Single wall carbon nanotubes (SWCNT) Quantization effects

Back gate Carbon nanotube Electrode Electrode L~300nm SiO2 (insulator) Conductance quantization: Gmax= 4 e2/h SWCNT (1nm): Four channels (Rmin= 26 k) Size quantization: E~1/L~ 1 meV (Wave nature of electron) Separated energy levels Charge quantization: Uc~e2/C~5 meV (Particle nature of electron) Single electron transport E SWCNT E+Uc

Outline

Single wall carbon nanotubes (SWCNT) Quantization effects SWCNT quantum dots

Device Fabrication

(a) (b) (c) (d) (e) (a) Alignment marks made using lithography and metal evaporation (b) Catalyst islands made using lithography and material spinning (c) Grow SWCNT by chemical vapour deposition (d) Electrodes made using electron beam lithography and metal evaporation (e) Bonding pads made using optical lithography and metal evaporation

Cryogenics – measurements at low temperature

Low temperature is needed to observe these quantum phenomena 4K: Helium bath (4He) 300mK Heliox: Closed liquid/gas system (3He) 30mK Kelvinox: 3He/4He dilution refrigerator

Measurement setup

Back gate Vgate Vsd SWCNT Two voltage knobs: Source-drain voltage Vsd Gate voltage

Uc ΔE μs μd Coulomb blockade and single electron tunneling Vg[V] G[e2/h] 2 3 4 5 1 2x Coulomb Blockade Single electron tunneling

Vsd[mV] Uc 3 2 1 ΔE 5 4 Uc/(eα) Uc Uc ΔE μs μd eVsd White: High dI/dV (increase in current) Black: Low dI/dV

Outline

Single wall carbon nanotubes (SWCNT) Quantization effects SWCNT quantum dots The Kondo effect in bulk

Kondo effect causes increased resistivity at low temperatures

Kondo Effect in bulk Kondo cloud at low temperature

Outline

Single wall carbon nanotubes (SWCNT) Quantization effects SWCNT quantum dots The Kondo effect in bulk Kondo effects in carbon nanotubes Equilibrium (Zero bias)

Spin on Tube Kondo Cloud in Electrodes Kondo effect with odd occupancy on tube

Spin flipping proces

(a) Uc (b) (c) x x x x Odd Odd Odd Odd Even Even Even Even Δt ~ h/Uc

Extra peak in density of states

μs μd Γ Γs Γd μs μd Γ Γs Γd ε0 ε0 N is odd N is even Γ= Γs + Γd ~2kBTK

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Name: 
Master Colloqvium
Author: 
Jeppe Holm
Company: 
Nanolab
Description: 
Kondo Effects in Carbon Nanotubes Master Colloquium by Jeppe Vilstrup Holm Supervisor: Poul Erik Lindelof
Tags: 
effect | odd | swcnt | kondo | carbon | nanotub | singl | quantiz
Created: 
2/6/2007 10:27:21 AM
Slides: 
28
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