scholarly journals Origins of Leakage Currents on Electrolyte-Gated Graphene Field-Effect Transistors

Author(s):  
Anastasia Svetlova ◽  
Dmitry Kireev ◽  
Guillermo Beltramo ◽  
Dirk Mayer ◽  
Andreas Offenhäusser
2004 ◽  
Vol 14 (01) ◽  
pp. 197-224 ◽  
Author(s):  
G. SIMIN ◽  
M. ASIF KHAN ◽  
M. S. SHUR ◽  
R. GASKA

Unique materials properties of GaN -based semiconductors that make them promising for high-power high-temperature applications are high electron mobility and saturation velocity, high sheet carrier concentration at heterojunction interfaces, high breakdown field, and low thermal impedance (when grown over SiC or bulk AlN substrates). The chemical inertness of nitrides is another key property. An AlGaN / GaN Heterostructure Field Effect Transistor (HFET) has been a topic of intensive investigations since the first report in 1991 [1]. Several groups demonstrated high power operation of AlGaN / GaN HFETs at microwave frequencies [2,3,4], including a 100 W output power single chip amplifier developed by Cree, Inc. and devices with 100 GHz cut-off frequency reported in [5]. However, in spite of impressive achievements, the potential of nitride based HFETs has not been fully realized as yet. The RF powers expected from the fundamental properties of nitride based materials significantly exceed the experimental data. One of the key problems limiting the HFETs RF characteristics is high gate leakage currents causing DC and RF parameter degradation. When the gate voltage goes positive the forward leakage current shunts the gate-channel capacitance and thus limits the maximum device current. When the gate voltage is negative, high voltage drop between the gate and the drain causes premature breakdown and thus limits maximum applied drain voltage. In addition, gate leakage currents increase the device sub-threshold currents, which decrease the achievable amplitude of the RF output. These limitations become even more severe at high ambient temperatures. The characteristics of III-N HFETs can be considerably improved by implementing a new approach, which results from the demonstration of good quality of SiO 2/ AlGaN and Si 3 N 4/ AlGaN interfaces. This approach opens up a way to fabricate insulated gate heterostructure field-effect transistors (IGHFETs), which have the gate leakage currents several orders of magnitude below those of regular HFETs, and exhibit better linearity and higher channel saturation currents. In this chapter, we describe design, characterization and applications of these novel devices.


2020 ◽  
Vol 11 (1) ◽  
Author(s):  
Qilin Hua ◽  
Guoyun Gao ◽  
Chunsheng Jiang ◽  
Jinran Yu ◽  
Junlu Sun ◽  
...  

AbstractPower dissipation is a fundamental issue for future chip-based electronics. As promising channel materials, two-dimensional semiconductors show excellent capabilities of scaling dimensions and reducing off-state currents. However, field-effect transistors based on two-dimensional materials are still confronted with the fundamental thermionic limitation of the subthreshold swing of 60 mV decade−1 at room temperature. Here, we present an atomic threshold-switching field-effect transistor constructed by integrating a metal filamentary threshold switch with a two-dimensional MoS2 channel, and obtain abrupt steepness in the turn-on characteristics and 4.5 mV decade−1 subthreshold swing (over five decades). This is achieved by using the negative differential resistance effect from the threshold switch to induce an internal voltage amplification across the MoS2 channel. Notably, in such devices, the simultaneous achievement of efficient electrostatics, very small sub-thermionic subthreshold swings, and ultralow leakage currents, would be highly desirable for next-generation energy-efficient integrated circuits and ultralow-power applications.


ACS Nano ◽  
2016 ◽  
Vol 10 (9) ◽  
pp. 8457-8464 ◽  
Author(s):  
Chaitanya U. Kshirsagar ◽  
Weichao Xu ◽  
Yang Su ◽  
Matthew C. Robbins ◽  
Chris H. Kim ◽  
...  

1996 ◽  
Vol 69 (9) ◽  
pp. 1229-1231 ◽  
Author(s):  
Zhifang Fan ◽  
S. N. Mohammad ◽  
Ö. Aktas ◽  
A. E. Botchkarev ◽  
A. Salvador ◽  
...  

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