Multiscale modeling of defect-related phenomena in high-k based logic and memory devices

Author(s):  
Andrea Padovani ◽  
Luca Larcher ◽  
Francesco Maria Puglisi ◽  
Paolo Pavan

2009 ◽  
Vol 45 (16) ◽  
pp. 821 ◽  
Author(s):  
K. Prashanthi ◽  
S.P. Duttagupta ◽  
R. Pinto ◽  
V.R. Palkar


2010 ◽  
Vol 87 (5-8) ◽  
pp. 1629-1633 ◽  
Author(s):  
J. Paul ◽  
V. Beyer ◽  
M. Czernohorsky ◽  
M.F. Beug ◽  
K. Biedermann ◽  
...  


Author(s):  
G. Gay ◽  
G. Molas ◽  
M. Bocquet ◽  
E. Jalaguier ◽  
M. Gely ◽  
...  


2009 ◽  
Vol 86 (7-9) ◽  
pp. 1789-1795 ◽  
Author(s):  
J.A. Kittl ◽  
K. Opsomer ◽  
M. Popovici ◽  
N. Menou ◽  
B. Kaczer ◽  
...  


2004 ◽  
Vol 830 ◽  
Author(s):  
Ch. Sargentis ◽  
K. Giannakopoulos ◽  
A. Travlos ◽  
D. Tsamakis

ABSTRACTMOS memory devices containing semiconductor nanocrystals have drawn considerable attention recently, due to their advantages when compared to the conventional memories. Only little work has been done on memory devices containing metal nanoparticles.We describe the fabrication of a novel MOS device with embedded Pt nanoparticles in the HfO2 / SiO2 interface of a MOS device. Using as control oxide, a high-k dielectric, our device has a great degree of scalability. The fabricated nanoparticles are very small (about 5 nm) and have high density. High frequency C-V measurements demonstrate that this device operates as a memory device.



2016 ◽  
Vol 30 (15) ◽  
pp. 1650279 ◽  
Author(s):  
Jinqiu Liu ◽  
Jianxin Lu ◽  
Jiang Yin ◽  
Bo Xu ◽  
Yidong Xia ◽  
...  

The charge-trapping memory devices namely Pt/Al2O3/(Al2O[Formula: see text](Cu2O)[Formula: see text]/SiO2/[Formula: see text]-Si with 2, 3 and 4 nm SiO2 tunneling layers were fabricated by using RF magnetron sputtering and atomic layer deposition techniques. At an applied voltage of ±11 V, the memory windows in the C–V curves of the memory devices with 2, 3 and 4 nm SiO2 tunneling layers were about 4.18, 9.91 and 11.33 V, respectively. The anomaly in memory properties among the three memory devices was ascribed to the different back tunneling probabilities of trapped electrons in the charge-trapping dielectric (Al2O[Formula: see text](Cu2O)[Formula: see text] due to the different thicknesses of SiO2 tunneling layer.



2007 ◽  
Vol 54 (10) ◽  
pp. 2699-2705 ◽  
Author(s):  
Ying Qian Wang ◽  
Wan Sik Hwang ◽  
Gang Zhang ◽  
G. Samudra ◽  
Yee-Chia Yeo ◽  
...  




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