4.8 Article

A Steep-Slope MoS2/Graphene Dirac-Source Field-Effect Transistor with a Large Drive Current

期刊

NANO LETTERS
卷 21, 期 4, 页码 1758-1764

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acs.nanolett.0c04657

关键词

MoS2; graphene; Dirac-source; gate-all-around; steep-slope; large drive current

资金

  1. National Natural Science Foundation of China [61925402, 61851402, 61734003]
  2. Science and Technology Commission of Shanghai Municipality [19JC1416600]
  3. National Key Research and Development Program [2017YFB0405600]
  4. Shanghai Education Development Foundation
  5. Shanghai Municipal Education Commission Shuguang Program [18SG01]
  6. China Postdoctoral Science Foundation [2019M661358, 2019TQ0065]

向作者/读者索取更多资源

In the process of continuously scaling transistor feature sizes, a transistor with a new mechanism is needed to break through the thermionic limit of subthreshold swing (SS) while maintaining a large drive current. By adopting the Dirac-source field-effect transistor (DSFET) technology, a MoS2/graphene DSFET is experimentally demonstrated for the first time, showing a steep SS and bringing in gate-all-around (GAA) structure further improves the transistor's performance in terms of SS and drive current, making it suitable for low-power and high-performance electronics applications.
In the continuous transistor feature size scaling down, the scaling of the supply voltage is stagnant because of the subthreshold swing (SS) limit. A transistor with a new mechanism is needed to break through the thermionic limit of SS and hold the large drive current at the same time. Here, by adopting the recently proposed Dirac-source field-effect transistor (DSFET) technology, we experimentally demonstrate a MoS2/graphene (1.8 nm/0.3 nm) DSFET for the first time, and a steep SS of 37.9 mV/dec at room temperature with nearly free hysteresis is observed. Besides, by bringing in the structure of gate-all-around (GAA), the MoS2/graphene DSFET exhibits a steeper SS of 33.5 mV/dec and a 40% increased normalized drive current up to 52.7 mu A.mu m/(V-DS = 1 V) with a current on/off ratio of 10(8), which shows potential for low-power and high-performance electronics applications.

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