High-k gate stack on germanium substrate with fluorine incorporation

2008 ◽  
Vol 92 (16) ◽  
pp. 163505 ◽  
Author(s):  
Ruilong Xie ◽  
Mingbin Yu ◽  
Mei Ying Lai ◽  
Lap Chan ◽  
Chunxiang Zhu
MRS Advances ◽  
2017 ◽  
Vol 2 (52) ◽  
pp. 2973-2982 ◽  
Author(s):  
Andreas Kerber

ABSTRACTMG/HK was introduced into CMOS technology and enabled scaling beyond the 45/32nm technology node. The change in gate stack from poly-Si/SiON to MG/HK introduced new reliability challenges like the positive bias temperature instability (PBTI) and stress induced leakage currents (SILC) in nFET devices which prompted thorough investigation to provide fundamental understanding of these degradation mechanisms and are nowadays well understood. The shift to a dual-layer gate stack also had a profound impact on the time dependent dielectric breakdown (TDDB) introducing a strong polarity dependence in the model parameter. As device scaling continues, stochastic modeling of variability, both at time zero and post stress due to BTI, becomes critical especially for SRAM circuit aging. As we migrate towards novel device architectures like bulk FinFET, SOI FinFETs, FDSOI and gate-all-around devices, impact of self-heating needs to be accounted for in reliability testing.In this paper we summarize the fundamentals of MG/HK reliability and discuss the reliability and characterization challenges related to the scaling of future CMOS technologies.


2011 ◽  
Vol 88 (7) ◽  
pp. 1488-1491 ◽  
Author(s):  
A.J. Craven ◽  
B. Schaffer ◽  
M.C. Sarahan
Keyword(s):  

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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