scholarly journals Subthreshold Analytical Model of Asymmetric Gate Stack Triple Metal Gate all Around MOSFET (AGSTMGAAFET) for Improved Analog Applications

Silicon ◽  
2021 ◽  
Author(s):  
Arvind Ganesh ◽  
Kshitij Goel ◽  
Jaskeerat Singh Mayall ◽  
Sonam Rewari
2021 ◽  
Author(s):  
Arvind Ganesh ◽  
Kshitij Goel ◽  
Jaskeerat Singh Mayall ◽  
Sonam Rewari

Abstract In this paper, we have proposed a 2D analytical model for Asymmetric gate stack triple metal gate MOSFET(AGSTMGAAFET) and performed a comparative analysis with the simulation results obtained using the SILVACO 3D simulation software. Existing devices such as gate all around single metal (SMGAAFET), gate all around triple metal (TMGAAFET), gate stack single metal (GSSMGAAFET), gate stack triple metal (GSTMGAAFET) and asymmetric gate stack single metal (AGSTMGAAFET) have been compared with our proposed structure AGSTMGAAFET. Our device provides excellent performance in terms of drain current, transconductance, output conductance, current gain, maximum transducer power gain which shows our device’s suitability for various analog applications moreover the potential and electric field plots obtained have twostep profile and extremely low electric field near the drain region which ordains our device with the ability to suppress various SCE’s like DIBL and hot-carrier effect. The analytical model and simulation results show good convergence in values which validate the correctness of the proposed model.


2019 ◽  
Vol 9 (11) ◽  
pp. 2388 ◽  
Author(s):  
Chao Zhao ◽  
Jinjuan Xiang

The continuous down-scaling of complementary metal oxide semiconductor (CMOS) field effect transistors (FETs) had been suffering two fateful technical issues, one relative to the thinning of gate dielectric and the other to the aggressive shortening of channel in last 20 years. To solve the first issue, the high-κ dielectric and metal gate technology had been induced to replace the conventional gate stack of silicon dioxide layer and poly-silicon. To suppress the short channel effects, device architecture had changed from planar bulk Si device to fully depleted silicon on insulator (FDSOI) and FinFETs, and will transit to gate all-around FETs (GAA-FETs). Different from the planar devices, the FinFETs and GAA-FETs have a 3D channel. The conventional high-κ/metal gate process using sputtering faces conformality difficulty, and all atomic layer deposition (ALD) of gate stack become necessary. This review covers both scientific and technological parts related to the ALD of metal gates including the concept of effect work function, the material selection, the precursors for the deposition, the threshold voltage (Vt) tuning of the metal gate in contact with HfO2/SiO2/Si. The ALD of n-type metal gate will be detailed systematically, based mainly on the authors’ works in last five years, and the all ALD gate stacks will be proposed for the future generations based on the learning.


2013 ◽  
Vol 88 ◽  
pp. 21-26 ◽  
Author(s):  
C. Leroux ◽  
S. Baudot ◽  
M. Charbonnier ◽  
A. Van Der Geest ◽  
P. Caubet ◽  
...  

2017 ◽  
Vol 38 (3) ◽  
pp. 379-382 ◽  
Author(s):  
C. Suarez-Segovia ◽  
C. Leroux ◽  
F. Domengie ◽  
G. Ghibaudo

2011 ◽  
Vol 1336 ◽  
Author(s):  
U. Celano ◽  
T. Conard ◽  
T. Hantschel ◽  
W. Vandervorst

ABSTRACTThe metal gate high k interaction is one of the dominant processes influencing the electrical performance (Vt, charge accumulation,..) of advanced gate stacks. These interactions are influenced by the entire thermal budget and the presence of reactive elements (on top/ within the material gate) such that relevant measurements can only be performed after a full processing cycle and on a complete gate stack.In such cases the relevant metal gate high k interface is a buried interface located below the metal gate (+ Si cap) and is not accessible for standard characterization methods like x-ray photoemission spectroscopy (XPS) due the limited escape depth of the photoelectrons. Moreover the presence of a conductive metal gate prevents the application of techniques such as conductive atomic force microscopy (C-AFM), to probe the local distribution of the defects, trapping sites and local degradation upon stressing. XPS in combination with layer removal steps like ion beam sputtering will destroy the bonding information and is thus not applicable. Chemical etching of the metal gate stack prior to the XPS measurements requires an extremely precious control of the etching in order to stop 1-2 nm before the high k metal interface.As an alternative we have developed a backside removal approach, that allows us to investigate using techniques such as XPS and C-AFM, the metal gate high k interface.


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