The Role of Nonidealities in the Scaling of MoS2 FETs

被引:17
|
作者
Verreck, Devin [1 ]
Arutchelvan, Goutham [1 ,2 ]
Lockhart de la Rosa, Cesar J. [1 ]
Leonhardt, Alessandra [1 ,3 ]
Chiappe, Daniele [1 ]
Lu, Anh Khoa Augustin [4 ]
Pourtois, Geoffrey [1 ]
Matagne, Philippe [1 ]
Heyns, Marc M. [1 ,2 ]
De Gendt, Stefan [1 ,3 ]
Mocuta, Anda [1 ]
Radu, Iuliana P. [1 ]
机构
[1] Imec, B-3001 Leuven, Belgium
[2] Katholieke Univ Leuven, Dept Mat Engn, B-3001 Leuven, Belgium
[3] Katholieke Univ Leuven, Dept Chem, B-3001 Leuven, Belgium
[4] Tohoku Univ, Natl Inst Adv Ind Sci & Technol, Math Adv Mat Open Innovat Lab, Sendai, Miyagi 9808577, Japan
关键词
2-D semiconductors; transition metal dichalcogenides; MOLYBDENUM-DISULFIDE; WANNIER FUNCTIONS; TRANSISTORS; DEPOSITION; CONTACTS; LAYERS; FILMS; METAL;
D O I
10.1109/TED.2018.2863750
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
2-D material FETs hold the promise of excellent gate control, but the impact of nonidealities on their performance remains poorly understood. This is because of the need, so far, to use computationally intensive nonequilibrium Green'sf unction (NEGF) simulations. Here, we therefore use a semiclassical model to investigate the role of nonidealities in the scaling of back-gated (BG) and top-gated (TG) monolayer MoS2 FETs. We verify the electrostatics and transport of the semiclassical model with density functional theory-based NEGF simulations and calibrate nonidealities, such as interface traps (D-it) and Schottky contact barrier height (OBB) to experimental monolayer and bilayer MoS2 FETs. We find that among the nonidealities, A t has the strongest subthreshold swing impact with 70 mV/dec obtainable in BG devices for a D-it of 5 x 10(11) cm(-2) eV(-1), an equivalent oxide thickness (EOT) of 1 nm, and a channel length (L-ch) of 5 nm. For scaled EOT, phi(SB) only strongly impacts I-ON for the TG case, as the overlapping gate thins the Schottky barriers in the BG case. We show in TG devices that a spacer of only 5 nm results in a 1000-fold drop in I-ON because of the nonidealities. We propose positive spacer oxide charge as a solution and show that a charge density of above 10(13) m(-2) is required to fully recover the device performance.
引用
收藏
页码:4635 / 4640
页数:6
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