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Eliminating Gate-Voltage Hysteresis in
Suspended Single-Walled Carbon
Nanotube Field-Effect Transistors
Ajay Subramanian, Takushi Uda, and Y.K. Kato
Outline
Introduction
◦ Single-Walled Carbon Nanotubes
◦ Field-Effect Transistor Architecture and Synthesis
◦ What is Gate-Voltage Hysteresis?
Measurements and Processes
◦ Optical Measurement Setup
◦ Measurements and Results
◦ Photoluminescence vs Gate-Voltage
◦ Pressure Dependence and Air Recovery
◦ Environment Effects
Conclusions and Future Work
Single-Walled Carbon Nanotubes
(SWCNT)
• SWCNTs have unique mechanical and electronic properties that
make them attractive for innovative new science
• Notably, different chiralities of nanotubes correspond to metallic
and semiconducting electronic properties.
• SWCNTs have small dimension and direct band gap: potential
application in optoelectronics
Field-Effect Transistor Architecture
• FET devices take advantage of these
properties; trench architecture allows
for large photoluminescence.
• Si back gate allows for electrostatic
doping of charge carriers
What is hysteresis?
-Environmental conditions that affect
the gate dependence of various
properties
-Adsorbed water or hydroxyl groups
-How do we eliminate it?
Semiconducting SWCNT
-6 -4 -2 0 2 4 6
0
50n
100n
150n
Draincurrent(A)
Gate voltage (V)
-6 -4 -2 0 2 4 6
0.0
1.0µ
2.0µ
3.0µ
Draincurrent(A)
Gate voltage (V)
Metallic SWCNT
Nano lett. 3, 193 (2003), W. Kim et al
Outline
Introduction
◦ Single-Walled Carbon Nanotubes
◦ Field-Effect Transistor Architecture and Synthesis
◦ What is Gate-Voltage Hysteresis?
Measurements and Processes
◦ Optical Measurement Setup
◦ Measurements and Results
◦ Photoluminescence vs Gate-Voltage
◦ Pressure Dependence and Air Recovery
◦ Environment Effects
Conclusions and Future Work
The Vacuum Box
Modified Optical Microscopy Cryostat
◦ Create PCB
◦ Wire the inside of the cryostat
◦ Create wire connection from voltage box to cryostat
◦ Mount in the optical setup
Optical Setup
Lens
Shutter
Pinhole
Steering
Mirror
Lens pair
1D Stage
Objective lens
Cryostat
Long-pass filter
PL
Detector
Outline
Introduction
◦ Single-Walled Carbon Nanotubes
◦ Field-Effect Transistor Architecture and Synthesis
◦ What is Gate-Voltage Hysteresis?
Measurements and Processes
◦ Optical Measurement Setup
◦ Measurements and Results
◦ Photoluminescence vs Gate-Voltage
◦ Pressure Dependence and Air Recovery
◦ Environment Effects
Conclusions and Future Work
Photoluminescence vs. Voltage
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
-5 -4 -3 -2 -1 0 1 2 3 4 5
Gate-Voltage
(V)
NormalizedPL(arb.units)
In Air In Vacuum
• In air: clear hysteresis defined by two distinct peaks , quenching values
• In vacuum, PL quenches normally; measurements done on (9,7) SWCNT
Pressure Dependence
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
1.0e3 mbar (Air) 3.0 mbar
6.3e-6 mbar1.4e-3 mbar
1000 100 10 1 0.1 0.01 1E-3 1E-4 1E-5 1E-6
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
Hysteresis(V)
Pressure (mbar)
• In situ pressure dependence measurements done with TurboPump
• Method: Z, 2D, reflectivity position scans. Then, X PL scan, followed by PLV
Air Recovery
-5 -4 -3 -2 -1 0 1 2 3 4 5 -5 -4 -3 -2 -1 0 1 2 3 4 5-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPL
-5 -4 -3 -2 -1 0 1 2 3 4 5
• Hysteresis recovers after exposure to air; we observe clear increase over time
• How can we control it?
N2 Environment
0 200 400 600 800 1000 1200 1400
-0.05
0.00
0.05
0.10
0.15
0.20
0.25
1.8
2.0
2.2
2.4
2.6
2.8
3.0
3.2
3.4
3.6
Hysteresis(V)
Time (minutes)
N2
Exposure
Air Exposure
N2 Environment
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
-5 -4 -3 -2 -1 0 1 2 3 4 5
0.0
0.2
0.4
0.6
0.8
1.0
NormalizedPLIntensity
Gate-Voltage (V)
60 min. N2 5910 min. (4 days) N2
Conclusions, Challenges, Future Work
• Clear elimination of hysteresis in PLV in the new vacuum box setup
• Isolated cause of hysteresis to adsorbed atmospheric molecules, e.g.
water
What’s next?
• New gate-voltage dependence measurements
• Possible giant band gap renormalization

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gcurs presentation

  • 1. Eliminating Gate-Voltage Hysteresis in Suspended Single-Walled Carbon Nanotube Field-Effect Transistors Ajay Subramanian, Takushi Uda, and Y.K. Kato
  • 2. Outline Introduction ◦ Single-Walled Carbon Nanotubes ◦ Field-Effect Transistor Architecture and Synthesis ◦ What is Gate-Voltage Hysteresis? Measurements and Processes ◦ Optical Measurement Setup ◦ Measurements and Results ◦ Photoluminescence vs Gate-Voltage ◦ Pressure Dependence and Air Recovery ◦ Environment Effects Conclusions and Future Work
  • 3. Single-Walled Carbon Nanotubes (SWCNT) • SWCNTs have unique mechanical and electronic properties that make them attractive for innovative new science • Notably, different chiralities of nanotubes correspond to metallic and semiconducting electronic properties. • SWCNTs have small dimension and direct band gap: potential application in optoelectronics
  • 4. Field-Effect Transistor Architecture • FET devices take advantage of these properties; trench architecture allows for large photoluminescence. • Si back gate allows for electrostatic doping of charge carriers
  • 5. What is hysteresis? -Environmental conditions that affect the gate dependence of various properties -Adsorbed water or hydroxyl groups -How do we eliminate it? Semiconducting SWCNT -6 -4 -2 0 2 4 6 0 50n 100n 150n Draincurrent(A) Gate voltage (V) -6 -4 -2 0 2 4 6 0.0 1.0µ 2.0µ 3.0µ Draincurrent(A) Gate voltage (V) Metallic SWCNT Nano lett. 3, 193 (2003), W. Kim et al
  • 6. Outline Introduction ◦ Single-Walled Carbon Nanotubes ◦ Field-Effect Transistor Architecture and Synthesis ◦ What is Gate-Voltage Hysteresis? Measurements and Processes ◦ Optical Measurement Setup ◦ Measurements and Results ◦ Photoluminescence vs Gate-Voltage ◦ Pressure Dependence and Air Recovery ◦ Environment Effects Conclusions and Future Work
  • 7. The Vacuum Box Modified Optical Microscopy Cryostat ◦ Create PCB ◦ Wire the inside of the cryostat ◦ Create wire connection from voltage box to cryostat ◦ Mount in the optical setup
  • 8. Optical Setup Lens Shutter Pinhole Steering Mirror Lens pair 1D Stage Objective lens Cryostat Long-pass filter PL Detector
  • 9. Outline Introduction ◦ Single-Walled Carbon Nanotubes ◦ Field-Effect Transistor Architecture and Synthesis ◦ What is Gate-Voltage Hysteresis? Measurements and Processes ◦ Optical Measurement Setup ◦ Measurements and Results ◦ Photoluminescence vs Gate-Voltage ◦ Pressure Dependence and Air Recovery ◦ Environment Effects Conclusions and Future Work
  • 10. Photoluminescence vs. Voltage -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 -5 -4 -3 -2 -1 0 1 2 3 4 5 Gate-Voltage (V) NormalizedPL(arb.units) In Air In Vacuum • In air: clear hysteresis defined by two distinct peaks , quenching values • In vacuum, PL quenches normally; measurements done on (9,7) SWCNT
  • 11. Pressure Dependence -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) 1.0e3 mbar (Air) 3.0 mbar 6.3e-6 mbar1.4e-3 mbar 1000 100 10 1 0.1 0.01 1E-3 1E-4 1E-5 1E-6 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 Hysteresis(V) Pressure (mbar) • In situ pressure dependence measurements done with TurboPump • Method: Z, 2D, reflectivity position scans. Then, X PL scan, followed by PLV
  • 12. Air Recovery -5 -4 -3 -2 -1 0 1 2 3 4 5 -5 -4 -3 -2 -1 0 1 2 3 4 5-5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPL -5 -4 -3 -2 -1 0 1 2 3 4 5 • Hysteresis recovers after exposure to air; we observe clear increase over time • How can we control it?
  • 13. N2 Environment 0 200 400 600 800 1000 1200 1400 -0.05 0.00 0.05 0.10 0.15 0.20 0.25 1.8 2.0 2.2 2.4 2.6 2.8 3.0 3.2 3.4 3.6 Hysteresis(V) Time (minutes) N2 Exposure Air Exposure
  • 14. N2 Environment -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) -5 -4 -3 -2 -1 0 1 2 3 4 5 0.0 0.2 0.4 0.6 0.8 1.0 NormalizedPLIntensity Gate-Voltage (V) 60 min. N2 5910 min. (4 days) N2
  • 15. Conclusions, Challenges, Future Work • Clear elimination of hysteresis in PLV in the new vacuum box setup • Isolated cause of hysteresis to adsorbed atmospheric molecules, e.g. water What’s next? • New gate-voltage dependence measurements • Possible giant band gap renormalization