Charge Accumulation in MOS Structures with a Polysilicon Gate under Tunnel Injection

2018 ◽  
Vol 52 (13) ◽  
pp. 1732-1737
Author(s):  
O. V. Aleksandrov ◽  
A. N. Ageev ◽  
S. I. Zolotarev
1985 ◽  
Vol 32 (5) ◽  
pp. 918-925 ◽  
Author(s):  
Dah-Bin Kao ◽  
K.C. Saraswat ◽  
J.P. McVittie

2007 ◽  
Vol 47 (4-5) ◽  
pp. 626-630 ◽  
Author(s):  
V. Turchanikov ◽  
A. Nazarov ◽  
V. Lysenko ◽  
V. Ostahov ◽  
O. Winkler ◽  
...  

1990 ◽  
Vol 182 ◽  
Author(s):  
J. Lin ◽  
S. Batra ◽  
K. Park ◽  
J. Lee ◽  
S. Banerjee ◽  
...  

AbstractThis paper discusses the effects of dopant segregation and electron trapping on the capacitance-voltage characteristics of arsenic-implanted polysilicon and amorphous Si gate MOS structures fabricated with and without a TiSi2 layer. The effects of gate bias, annealing temperature, silicide formation and polysilicon grain microstructure on the C-V characteristics have also been studied. The results show that insufficient arsenic redistribution at 800°C, coupled with carrier trapping at polysilicon grain boundaries and dopant segregation in TiSi2 causes depletion effects in the polysilicon gate and in turn, an anomalous capacitance-voltage behavior. The depletion tends to increase the “effective” gate oxide thickness and thereby degrade MOS device performance. Higher temperature anneals (≥ 900°C) are sufficient to achieve degenerate doping in the polysilicon gates and avoid the depletion effects.


1990 ◽  
Vol 183 ◽  
Author(s):  
Masaaki Niwa ◽  
Minoru Onoda ◽  
Hiroshi Iwasaki ◽  
Robert Sinclair

AbstractThe morphology of SiO2/Si interfaces in a semiconductor LOCOS active area grown by several oxidation conditions has been studied, to compare the roughness of the interfaces observed by STM and HRTEM in particular. Samples consisted of typical MOS structures with a polysilicon gate/SiO2/Si(100). Hydrogen terminated Si surfaces were prepared by means of HF dipping for STM observations. The interface roughness of a “dry” oxide observed by HRTEM was slightly larger than that of a “wet” oxide. Good agreement could be found between STM and HRTEM for the wet oxide interfaces. As for the dry oxide interface, it was more difficult to obtain a reproducible STM image than for the wet oxide interface, but the reverse was true for HRTEM. During the HRTEM, high energy electrons damage the sample and reduce the oxide thickness, especially in the wet oxide samples.


1986 ◽  
Vol 93 (2) ◽  
pp. K215-K218
Author(s):  
R. Petrova ◽  
S. Grancharov

1996 ◽  
Vol 17 (3) ◽  
pp. 103-105 ◽  
Author(s):  
B. Ricco ◽  
R. Versari ◽  
D. Esseni

1985 ◽  
Vol 90 (1) ◽  
pp. 393-400
Author(s):  
N. A. Avdeev ◽  
Yu. E. Gabdin ◽  
V. A. Gurtov ◽  
S. N. Kuznetsov

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