Graphene Barristor, a Triode Device with a Gate-Controlled Schottky Barrier
By Heejun Yang, J. Heo, Seongjun Park, H. Song, D. Seo, Kyung‐Eun Byun, Philip Kim, Inkyeong Yoo, Hyun‐Jong Chung, Kinam Kim. Science, 2012
911 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/c31b94438d33d544b8915837259b2f582471b72e
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In Atomic and Molecular Physics, and Optics
- K. Novoselov
- A. Di Bartolomeo
- Takashi Taniguchi
- A. C. Castro Neto
- Filippo Giubileo
- A. Mishchenko
- Mark C. Hersam
- Lincoln J. Lauhon
In Materials Chemistry
- K. Novoselov
- Mark C. Hersam
- A. Di Bartolomeo
- A. C. Castro Neto
- Takashi Taniguchi
- Filippo Giubileo
- A. Mishchenko
- Vinod K. Sangwan
Citations in the corpus
- Emerging device applications for semiconducting two-dimensional transition metal dichalcogenides. (2014, background): “Likewise, a vertical heterojunction between a semimetal (graphene) and a semiconductor (MoS2) creates a two-dimensional Schottky barrier at the interface that can be tuned by a gate voltage.(161) This concept was extended further to create a functional inverter by vertical stacking n-type and p-type”
- Gate-tunable van der Waals heterostructure for reconfigurable neural network vision sensor (2020, background): “Two-dimensional (2D) materials with atomic thickness and flatness have shown great potential for numerous applications in electronics (14-17) and optoelectronics (18-20).”
- Tunable Schottky barrier and high responsivity in graphene/Si-nanotip optoelectronic device (2016, background): “or junctions if the Si-surface is defects-free and with saturated dangling bonds55. An ideal, trap free interface would result in unpinned Fermi level and yield a Schottky barrier height Φ�=Φ� −Χ�𝑖 , (11) (Schottky-Mott relation) in the range 0.45÷0.55 �� for undoped graphene. The Fermi level unpin”