Introduction
to Tunnel
Field Effect
Transistor
- Gadarapulla Rasheed
28-06-2024 1
Introduction to Tunnel FET
• Tunnel FET is a gated reverse biased P-I-N structure.
• Basic structure of TFET consists of source, channel and drain. Unlike
MOSFETs, the doping of the drain and the source are of opposite types in
a TFET.
• The current conduction mechanism of TFET is Band-to-Band Tunneling
(BTBT) whereas in a MOSFET, it is due to the thermionic emission of the
carrier over the potential barrier.
28-06-2024 2
VD > 0 V VS= 0
VGS > 0
VD < 0 V VS= 0
VGS < 0
The Concept of Tunneling
28-06-2024 3
Source: The Tunneling Transistor, by Alan Seabaugh (IEEE Spectrum, Oct 2013)
Energy Band Diagram of n-TFET
28-06-2024 4
Subthreshold Swing (SS)
28-06-2024 5
Transfer char. of MOSFET and Tunnel FET
[Ionescu A.M et al., Nature, 2011]
In a MOSFET,
SS = 1 +
𝐶𝑑
𝐶𝑜𝑥
ln(10)
𝑘𝑇
𝑞
SS ≈ 60 mV/decade @ 300 K
Subthreshold Swing (SS)=
𝑑𝑉𝐺𝑆
𝑑𝑙𝑜𝑔10𝐼𝐷
Subthreshold Slope =
1
𝑆𝑢𝑏𝑡ℎ𝑟𝑒𝑠ℎ𝑜𝑙𝑑 𝑆𝑤𝑖𝑛𝑔
due to Boltzmann distribution of charge carriers.
Features of Tunnel FET
 Very low OFF current (IOFF)
 Low ON current (ION)
 High ION/IOFF ratio
 Band-to-band tunnelling
 SS is not limited to 60mV/decade
28-06-2024 6
𝐼𝐷 ∝ exp −
4 2m∗𝐸𝑔
∗
3
2
3 𝑒 ℏ 𝐸𝑔
∗
+ ΔΦ
𝜀Si
𝜀ox
𝑡ox𝑡Si ΔΦ


















E
e
3
2
3
*
g
E
*
2m
4
exp
BTBT
T

Where,
m∗
- effective mass of charge
𝐸𝑔
∗
- effective energy bandgap
εsi, εox - permittivity of Si and oxide
tSi, tox- thickness of Si and oxide
ΔФ – Energy overlap window
E - Electric Field
Tunneling probability,
• Tunneling current is most sensitive to the effective
masses because the tunneling probability depends
exponentially on them.
28-06-2024 7
Thank You

Introduction to Tunnel Field Effect Transistor.pptx

  • 1.
    Introduction to Tunnel Field Effect Transistor -Gadarapulla Rasheed 28-06-2024 1
  • 2.
    Introduction to TunnelFET • Tunnel FET is a gated reverse biased P-I-N structure. • Basic structure of TFET consists of source, channel and drain. Unlike MOSFETs, the doping of the drain and the source are of opposite types in a TFET. • The current conduction mechanism of TFET is Band-to-Band Tunneling (BTBT) whereas in a MOSFET, it is due to the thermionic emission of the carrier over the potential barrier. 28-06-2024 2 VD > 0 V VS= 0 VGS > 0 VD < 0 V VS= 0 VGS < 0
  • 3.
    The Concept ofTunneling 28-06-2024 3 Source: The Tunneling Transistor, by Alan Seabaugh (IEEE Spectrum, Oct 2013)
  • 4.
    Energy Band Diagramof n-TFET 28-06-2024 4
  • 5.
    Subthreshold Swing (SS) 28-06-20245 Transfer char. of MOSFET and Tunnel FET [Ionescu A.M et al., Nature, 2011] In a MOSFET, SS = 1 + 𝐶𝑑 𝐶𝑜𝑥 ln(10) 𝑘𝑇 𝑞 SS ≈ 60 mV/decade @ 300 K Subthreshold Swing (SS)= 𝑑𝑉𝐺𝑆 𝑑𝑙𝑜𝑔10𝐼𝐷 Subthreshold Slope = 1 𝑆𝑢𝑏𝑡ℎ𝑟𝑒𝑠ℎ𝑜𝑙𝑑 𝑆𝑤𝑖𝑛𝑔 due to Boltzmann distribution of charge carriers.
  • 6.
    Features of TunnelFET  Very low OFF current (IOFF)  Low ON current (ION)  High ION/IOFF ratio  Band-to-band tunnelling  SS is not limited to 60mV/decade 28-06-2024 6 𝐼𝐷 ∝ exp − 4 2m∗𝐸𝑔 ∗ 3 2 3 𝑒 ℏ 𝐸𝑔 ∗ + ΔΦ 𝜀Si 𝜀ox 𝑡ox𝑡Si ΔΦ                   E e 3 2 3 * g E * 2m 4 exp BTBT T  Where, m∗ - effective mass of charge 𝐸𝑔 ∗ - effective energy bandgap εsi, εox - permittivity of Si and oxide tSi, tox- thickness of Si and oxide ΔФ – Energy overlap window E - Electric Field Tunneling probability, • Tunneling current is most sensitive to the effective masses because the tunneling probability depends exponentially on them.
  • 7.