Improving the quality of sub-1.5-nm-thick oxynitride gate dielectric for FETs with narrow channel and shallow-trench isolation using radical oxygen and nitrogen

2002 ◽  
Vol 49 (10) ◽  
pp. 1736-1741 ◽  
Author(s):  
M. Togo ◽  
K. Watanabe ◽  
M. Terai ◽  
T. Yamamoto ◽  
T. Fukai ◽  
...  
2010 ◽  
Vol 54 (5) ◽  
pp. 609-611
Author(s):  
H.J. Hung ◽  
J.B. Kuo ◽  
D. Chen ◽  
C.T. Tsai ◽  
C.S. Yeh

2018 ◽  
Vol 27 (2) ◽  
pp. 028501 ◽  
Author(s):  
Meng-Ying Zhang ◽  
Zhi-Yuan Hu ◽  
Da-Wei Bi ◽  
Li-Hua Dai ◽  
Zheng-Xuan Zhang

2002 ◽  
Vol 716 ◽  
Author(s):  
Parag C. Waghmare ◽  
Samadhan B. Patil ◽  
Rajiv O. Dusane ◽  
V.Ramgopal Rao

AbstractTo extend the scaling limit of thermal SiO2, in the ultra thin regime when the direct tunneling current becomes significant, members of our group embarked on a program to explore the potential of silicon nitride as an alternative gate dielectric. Silicon nitride can be deposited using several CVD methods and its properties significantly depend on the method of deposition. Although these CVD methods can give good physical properties, the electrical properties of devices made with CVD silicon nitride show very poor performance related to very poor interface, poor stability, presence of large quantity of bulk traps and high gate leakage current. We have employed the rather newly developed Hot Wire Chemical Vapor Deposition (HWCVD) technique to develop the a:SiN:H material. From the results of large number of optimization experiments we propose the atomic hydrogen of the substrate surface prior to deposition to improve the quality of gate dielectric. Our preliminary results of these efforts show a five times improvement in the fixed charges and interface state density.


1998 ◽  
Author(s):  
I. De Wolf ◽  
G. Groeseneken ◽  
H.E. Maes ◽  
M. Bolt ◽  
K. Barla ◽  
...  

Abstract It is shown, using micro-Raman spectroscopy, that Shallow Trench Isolation introduces high stresses in the active area of silicon devices when wet oxidation steps are used. These stresses result in defect formation in the active area, leading to high diode leakage currents. The stress levels are highest near the outer edges of line structures and at square structures. They also increase with decreasing active area dimensions.


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