Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Anisotropic transport in tellurene FETs

View through CrossRef
Tellurene, a single layer of tellurium, is a new emerging 2D material and a possible candidate for the post‐silicon era. It has anisotropic carrier effective mass in zigzag and armchair directions. Therefore, the study of the anisotropic performance of tellurene FETs is a timely topic. In this work, the authors study the transport mechanism and performance metrics of tellurene n‐channel and p‐channel transistors using a quantum simulation. Heavy carrier mass in the armchair direction effectively blocks the tunnelling current and the transport is governed by thermionic emission over the potential barrier. On the other hand, lighter carrier mass in the zigzag direction results in a mixed tunnelling and thermionic transport mechanism. The n‐channel transistor has an on‐state current of 894 μA/μm, a sub‐threshold slope of 62 mV/dec, a 9.27 mS/μm transconductance, a 0.129 ps delay, and a 0.046 fJ/μm dynamic power loss. The p‐channel metrics are, respectively, 852 μA/μm, 62 mV/dec, 9.24 mS/μm, 0.117 ps, and 0.040 fJ/μm. Both the transistors comply with the International Technology Roadmap for Semiconductors 2026 low operating power device requirements.
Institution of Engineering and Technology (IET)
Title: Anisotropic transport in tellurene FETs
Description:
Tellurene, a single layer of tellurium, is a new emerging 2D material and a possible candidate for the post‐silicon era.
It has anisotropic carrier effective mass in zigzag and armchair directions.
Therefore, the study of the anisotropic performance of tellurene FETs is a timely topic.
In this work, the authors study the transport mechanism and performance metrics of tellurene n‐channel and p‐channel transistors using a quantum simulation.
Heavy carrier mass in the armchair direction effectively blocks the tunnelling current and the transport is governed by thermionic emission over the potential barrier.
On the other hand, lighter carrier mass in the zigzag direction results in a mixed tunnelling and thermionic transport mechanism.
The n‐channel transistor has an on‐state current of 894 μA/μm, a sub‐threshold slope of 62 mV/dec, a 9.
27 mS/μm transconductance, a 0.
129 ps delay, and a 0.
046 fJ/μm dynamic power loss.
The p‐channel metrics are, respectively, 852 μA/μm, 62 mV/dec, 9.
24 mS/μm, 0.
117 ps, and 0.
040 fJ/μm.
Both the transistors comply with the International Technology Roadmap for Semiconductors 2026 low operating power device requirements.

Related Results

First-principles study of electronic structure and optical properties of monolayer defective tellurene
First-principles study of electronic structure and optical properties of monolayer defective tellurene
Monolayer tellurene is a novel two-dimensional semiconductor with excellent intrinsic properties. It is helpful in understanding doping and scattering mechanism to study the electr...
Carbon nanotube and graphene field-effect transistors for aptamer and odorant receptor-based biosensors
Carbon nanotube and graphene field-effect transistors for aptamer and odorant receptor-based biosensors
<p>Carbon nanotubes (CNTs) and graphene field-effect transistors (FETs) are investigated here for their utility as sensors incorporating aptamers and insect odorant receptors...
Review on Perovskite Semiconductor Field–Effect Transistors and Their Applications
Review on Perovskite Semiconductor Field–Effect Transistors and Their Applications
Perovskite materials are considered as the most alluring successor to the conventional semiconductor materials to fabricate solar cells, light emitting diodes and electronic displa...
Air Processed Cs2AgBiBr6 Lead-free Double Perovskite High-mobility Thin Film Field-effect Transistors
Air Processed Cs2AgBiBr6 Lead-free Double Perovskite High-mobility Thin Film Field-effect Transistors
Abstract This study focuses on the fabrication and characterization of Cs2AgBiBr6 double perovskite thin film for field-effect transistor (FET) applications. The Cs2AgBiBr6...
Tunable Sub-THz and THz Lasing Effect Using FETs at Room Temperature
Tunable Sub-THz and THz Lasing Effect Using FETs at Room Temperature
I report on the first observed self-amplification by stimulated emission of 0.2THz and 1.63THz radiation using InGaAs/GaAs HEMT operating in the deep saturation regime at room temp...
Research on Approval of Domestic and International Transport Container Application of Radioactive Material
Research on Approval of Domestic and International Transport Container Application of Radioactive Material
Due to the potentially dangerous properties of radioactive material, it is during the transport that the process of nuclear energy and technology uses are prone to nuclear and radi...
Dynamic Lattice Method for Elastic Wave Simulation in 3-dimensional Arbitrary Anisotropic Media
Dynamic Lattice Method for Elastic Wave Simulation in 3-dimensional Arbitrary Anisotropic Media
To simulate the elastic wave propagations in 3-dimensional (3D) anisotropic media, a 3D anisotropic lattice model is proposed. The derivation of the general relationship between th...

Back to Top