Effect of Ti Substrate Ion Implantation on the Physical Properties of Anodic TiO2 Nanotubes

2018 ◽  
Vol 72 (5) ◽  
pp. 604-609 ◽  
Author(s):  
Zahra Jedi-Soltanabadi ◽  
Mahmood Ghoranneviss ◽  
Zohreh Ghorannevis ◽  
Hossein Akbari
1996 ◽  
Vol 46 (S3) ◽  
pp. 1479-1480
Author(s):  
Vasilij Šmatko ◽  
Pavol Čičmanec ◽  
František Hanic ◽  
Vladimír Štrbík ◽  
Štefan Beňačka ◽  
...  

Author(s):  
J. Narayan ◽  
D. Fathy

The structure of amorphous silicon determines its physical properties ranging from crystallization kinetics to efficiency of solar cells. One point of particular interest has been the existance of microcrystallites in the amorphous phase. Different crystallization kinetics are obtained for purely amorphous silicon and for amorphous silicon having a trace of crystallinity. The incorporation of dopants into substitutional sites after solid-phase crystallization has been also found to be affected by the degree of amorphousness.The purpose of this investigation was two fold: first, to characterize the structure of amorphous silicon, and second to study the structure of amorphous-crystalline interface. The importance of these two factors in the crystallization phenomena is discussed.


2018 ◽  
Vol 9 ◽  
pp. 1246-1249 ◽  
Author(s):  
Negin Pishkar ◽  
Mahmood Ghoranneviss ◽  
Zohreh Ghorannevis ◽  
Hossein Akbari

1983 ◽  
Vol 27 ◽  
Author(s):  
H.B. Dietrich ◽  
R.J. Corazzi ◽  
W.F. Tseng

AbstractSubstrates can undergo major temperature excursions during ion implantation if they are not well heat sunk. At power densities on the order of 50 watts per cm−2 radiatively cooled Si will melt in a matter of seconds. Such power densities can be maintained over a few sq. cms with many of the beams produced by even the moderate current machines currently used for doping Si and the III-V's. We have made use of this fact to study pulsed ion-beam annealing of implanted Si. Two types of studies have been carried out. In the first, 5–20 sec proton irradiations were done at power densities of 3–35 watts cm−2 to produce sample temperatures of 500 to 1100°C. 2×1016 cm−2 280 keV B, BF2 , As and P implants were annealed in this manner. Sheet resistances, ρs, versus power density curves were obtained for each ion and compared to psρs vs T data obtained for furnace annealed companion samples. In the second study the 2×1016cm−2 280 keV implants were carried out at progressively higher current densities so that the dopant beam itself raised the sample temperature to 500–1000°C. For each ion (other than B) it was possible to obtain power densities which resulted in self-annealing implants whose sheet resistances were as low as those obtained with the optimal furnace anneal. Details of the experiments, electrical and physical properties of the pulsed ion-beam annealed layers and device applications will be presented in this paper.


Author(s):  
Jane G. Zhu ◽  
C. W. White ◽  
S. P. Withrow ◽  
J. D. Budai ◽  
R. Mu ◽  
...  

2015 ◽  
Vol 161 ◽  
pp. 309-312 ◽  
Author(s):  
Xinggang Hou ◽  
Dong Mao ◽  
Huiyan Ma ◽  
Yukai Ai ◽  
Xinlei Zhao ◽  
...  

2012 ◽  
Vol 61 (10) ◽  
pp. 105203
Author(s):  
Huang Yong-Xian ◽  
L Shi-Xiong ◽  
Tian Xiu-Bo ◽  
Yang Shi-Qin ◽  
Fu Ricky ◽  
...  

2016 ◽  
Vol 128 (11) ◽  
pp. 3827-3831 ◽  
Author(s):  
Xuemei Zhou ◽  
Volker Häublein ◽  
Ning Liu ◽  
Nhat Truong Nguyen ◽  
Eva M. Zolnhofer ◽  
...  

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