ti nanolayer
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Wear ◽  
2021 ◽  
pp. 203798
Author(s):  
M. Alvarez-Vera ◽  
H.M. Hdz-García ◽  
J.C. Díaz-Guillén ◽  
R. Muñoz-Arroyo ◽  
J.L. Acevedo-Davila ◽  
...  

2019 ◽  
Vol 58 (6) ◽  
pp. 065502
Author(s):  
Eita Kudo ◽  
Midori Kawamura ◽  
Takayuki Kiba ◽  
Yoshio Abe ◽  
Kyung Ho Kim ◽  
...  
Keyword(s):  

2016 ◽  
Vol 50 (3) ◽  
pp. 411-414
Author(s):  
A. A. Yugov ◽  
S. S. Malahov ◽  
A. A. Donskov ◽  
M. P. Duhnovskii ◽  
S. N. Knyazev ◽  
...  

2015 ◽  
Vol 1729 ◽  
pp. 59-64
Author(s):  
P. Bousoulas ◽  
I. Michelakaki ◽  
J. Giannopoulos ◽  
K. Giannakopoulos ◽  
D. Tsoukalas

ABSTRACTWe present a detailed study of memory performance of titanium oxide (TiO2-x)-based resistive switching memories by modifying critical parameters of the films involved in the memory stack grown by reactive sputtering at room temperature. The device includes a Ti nanolayer at the Au/TiO2-x interface and it is defined by the following material stack: Au/Ti/TiO2-x/Au/SiO2/Si. We investigate the memory performance optimization of the device in terms of the Ti nanolayer thickness using as a starting point for the TiO2-x growth conditions these identified by varying the ratio of oxygen concentration to argon concentration by our previous results. Due to the superb ability of Ti to absorb oxygen atoms from the dielectric matrix, a large amount of oxygen vacancies is created, which are crucial for the stable function of the memory devices. We observe the existence of an optimum Ti thickness that if further increased gradually degrades the resistive switching behavior. The induced interface oxide thickness is found also to affect the fluctuation of the ON/OFF processes. In terms of electrical performance self-rectifying characteristics were recorded for all samples in the both resistance states. We then demonstrate that at least five-level resistance states could be obtained by modifying the compliance current, exhibiting excellent resistance uniformity and retention capability. The results are supported by C-AFM measurements demonstrating the scaling potential of the large area device discussed above.


2014 ◽  
Vol 9 (1) ◽  
pp. 125 ◽  
Author(s):  
Amit Prakash ◽  
Siddheswar Maikap ◽  
Hsien-Chin Chiu ◽  
Ta-Chang Tien ◽  
Chao-Sung Lai

2013 ◽  
Vol 8 (1) ◽  
pp. 288 ◽  
Author(s):  
Amit Prakash ◽  
Siddheswar Maikap ◽  
Hsien-Chin Chiu ◽  
Ta-Chang Tien ◽  
Chao-Sung Lai

2013 ◽  
Vol 8 (1) ◽  
pp. 419 ◽  
Author(s):  
Amit Prakash ◽  
Siddheswar Maikap ◽  
Hsien-Chin Chiu ◽  
Ta-Chang Tien ◽  
Chao-Sung Lai

2012 ◽  
Vol 7 (1) ◽  
pp. 345 ◽  
Author(s):  
Sheikh Rahaman ◽  
Siddheswar Maikap ◽  
Ta-Chang Tien ◽  
Heng-Yuan Lee ◽  
Wei-Su Chen ◽  
...  

1993 ◽  
Vol 308 ◽  
Author(s):  
H. Kung ◽  
M. Nastasi ◽  
T. R. Jervis ◽  
K.M. Hubbard ◽  
R.M. Messner ◽  
...  

ABSTRACTMultilayers of Ru-Cu and Ru-Ti have been prepared by electron beam evaporation technique. One set of composites has Ru thickness varying from 250 to 2500Å alternating with Cu or Ti of 15Å. The other set has 250Å of Ru and the Cu or Ti layer varies between 15 and 200Å. Nanoindentation measurements show that there is no significant change in hardness as either Ru or Cu/Ti thickness varies. However, the Ru-Cu multilayer has twice the hardness of the Ru-Ti system. High resolution transmission electron microscopy discloses that there is an epitaxial orientation relationship between Ru and Ti in Ru-Ti while no such relationship exists in Ru-Cu.The strengthening mechanism proposed by Koehler [1] predicts that Ru-Ti composites should have a higher strength than Ru-Cu due to the larger modulus difference between Ru and Ti. The discrepancy between the prediction and the experimental results suggests that other strengthening mechanism(s) may be operating. We have proposed two models based on a "shear" mechanism to explain the differences observed between these two systems. The effects of these mechanisms in controlling the deformation process in nanolayer composites are discussed.


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