Dependence of the Physical Properties of GaZnO/Polyethersulfoneon the Ar Gas Flow Rate During Sputtering Deposition Process

2009 ◽  
Vol 55 (2) ◽  
pp. 585-589 ◽  
Author(s):  
Junje Seong ◽  
DeukYoung Kim ◽  
Sejoon Lee
2011 ◽  
Vol 383-390 ◽  
pp. 903-908
Author(s):  
S. Shanmugan ◽  
D. Mutharasu ◽  
Z. Hassan ◽  
H. Abu. Hassan

Al thin films were prepared over different substrates at various process conditions using DC sputtering. The surface topography of all prepared films was examined using AFM technique. Very smooth, uniform and dense surface were observed for Al films coated over Glass substrates. The observed particle size was nano scale (20 -70 nm) for Glass substrates. Sputtering power showed immense effect on surface roughness with respective to Ar gas flow rate. Noticeable change on surface with large particles was observed in Copper substrates at various sputtering power and gas flow rate.


2017 ◽  
Vol 62 (2) ◽  
pp. 1119-1124
Author(s):  
B. Ali ◽  
S.H. Choi ◽  
S.J. Seo ◽  
D.Y. Maeng ◽  
C.G. Lee ◽  
...  

AbstractThe water atomization of iron powder with a composition of Fe-3Cr-0.5Mo (wt.%) at 1600°C and 150 bar creates an oxide layer, which in this study was reduced using a mixture of methane (CH4) and argon (Ar) gas. The lowest oxygen content was achieved with a 100 cc/min flow rate of CH4, but this also resulted in a co-deposition of carbon due to the cracking of CH4. This carbon can be used directly to create high-quality, sinter hardenable steel, thereby eliminating the need for an additional mixing step prior to sintering. An exponential relationship was found to exist between the CH4gas flow rate and carbon content of the powder, meaning that its composition can be easily controlled to suit a variety of different applications.


2012 ◽  
Vol 37 (2) ◽  
pp. 165-168 ◽  
Author(s):  
Iping Suhariadi ◽  
Naho Itagaki ◽  
Kazunari Kuwahara ◽  
Koichi Oshikawa ◽  
Daisuke Yamashita ◽  
...  

2012 ◽  
Vol 16 (5) ◽  
pp. 1544-1548
Author(s):  
Sheng Liu ◽  
Ying-Li Hao

Cold state experiment and numerical simulation are carried out to study particle deposition process. The deposit mass can be divided into two parts, one directly collides with the wall and the other is brought by the backflow. The deposit flux increases with the increase of gas flow rate or water flow rate or both, and decreases with the increase of the central channel gas flow rate.


2007 ◽  
Vol 1057 ◽  
Author(s):  
Yoshiyuki Suda ◽  
Junichi Takayama ◽  
Takeshi Saito ◽  
Atsushi Okita ◽  
Junji Nakamura ◽  
...  

ABSTRACTWe report the effect of CO2 addition to CO4 gas on carbon nanotube (CNT) growth by chemical vapor deposition. CO2 gas was introduced during the growth of CNTs on Fe0.05Mo0.025MgO0.925 and Ni0.05Mo0.025MgO0.925 catalysts by CO4 gas at a temperature of 800–850°C, and its concentration in a fraction of the gas flow rate was varied from 5×10−3 to 50%. In the experimental condition of the preferential growth of multi-walled CNTs, the carbon yield and the G/D ratio in the Raman spectra of the CNTs grown in 10%-CO2/CO4 were slightly higher than that grown in CO4 only. However, CNTs hardly grew when the CO2 concentration was more than 10%. We then prepared CO2 gas diluted with Ar gas (CO2/Ar) and varied its flow rate between 0 and 10 sccm. As the CO2/Ar gas flow rate was increased, the number of RBM peaks decreased even though the G/D ratio gradually decreased. The decrease in the RBM intensities of CNTs on the FeMoMgO catalyst was more significant than that of NiMoMgO.


2008 ◽  
Vol 202 (22-23) ◽  
pp. 5259-5261 ◽  
Author(s):  
Yongsup Yun ◽  
Takanori Yoshida ◽  
Norifumi Shimazu ◽  
Naoki Nanba ◽  
Yasushi Inoue ◽  
...  
Keyword(s):  
Gas Flow ◽  

2006 ◽  
Vol 911 ◽  
Author(s):  
Govindhan Dhanaraj ◽  
Yi Chen ◽  
Hui Chen ◽  
William M Vetter ◽  
Hui Zhang ◽  
...  

AbstractSiC homo-epitaxial layers were grown in a chemical vapor deposition process using silicon tetrachloride and propane precursors with hydrogen as a carrier gas. Growth rates were found to increase as temperatures increased at high carrier gas flow rate, while at lower carrier gas flow rate growth rates were observed to decrease as temperature increased. Based on the equilibrium model, “thermodynamically controlled growth” accounts for the growth rate reduction. The grown epitaxial layers were characterized using various techniques. Reduction in the threading screw dislocation (SD) density in the epilayers was observed. Suitable models were developed for explaining the reduction in the screw dislocation density as well as the conversion of basal plane dislocations (BPD) into threading edge dislocations (TED).


Nanomaterials ◽  
2021 ◽  
Vol 11 (7) ◽  
pp. 1635
Author(s):  
Md. Akhtaruzzaman ◽  
Md. Shahiduzzaman ◽  
Nowshad Amin ◽  
Ghulam Muhammad ◽  
Mohammad Aminul Islam ◽  
...  

Tungsten disulfide (WS2) thin films were deposited on soda-lime glass (SLG) substrates using radio frequency (RF) magnetron sputtering at different Ar flow rates (3 to 7 sccm). The effect of Ar flow rates on the structural, morphology, and electrical properties of the WS2 thin films was investigated thoroughly. Structural analysis exhibited that all the as-grown films showed the highest peak at (101) plane corresponds to rhombohedral phase. The crystalline size of the film ranged from 11.2 to 35.6 nm, while dislocation density ranged from 7.8 × 1014 to 26.29 × 1015 lines/m2. All these findings indicate that as-grown WS2 films are induced with various degrees of defects, which were visible in the FESEM images. FESEM images also identified the distorted crystallographic structure for all the films except the film deposited at 5 sccm of Ar gas flow rate. EDX analysis found that all the films were having a sulfur deficit and suggested that WS2 thin film bears edge defects in its structure. Further, electrical analysis confirms that tailoring of structural defects in WS2 thin film can be possible by the varying Ar gas flow rates. All these findings articulate that Ar gas flow rate is one of the important process parameters in RF magnetron sputtering that could affect the morphology, electrical properties, and structural properties of WS2 thin film. Finally, the simulation study validates the experimental results and encourages the use of WS2 as a buffer layer of CdTe-based solar cells.


2020 ◽  
Vol 62 (1) ◽  
pp. 46
Author(s):  
К.Х. Нусупов ◽  
Н.Б. Бейсенханов ◽  
Д.И. Бакранова ◽  
С. Кейнбай ◽  
А.А. Турахун ◽  
...  

Abstract The influence of deposition parameters, such as: the magnetron power in the range 690–1400 W, the silicon substrate temperature 23–170°C, the N_2 gas flow rate 0.9–3.6 L/h, the Ar gas flow rate 0.06‒3.6 L/h, the ratio of N_2/Ar gas flows 1–60 on the thickness, the density, and the composition of the deposited films is analyzed. The maximum density 5.247 g/cm^3 corresponding to the TiN_0.786 = Ti_56N_44 composition has been achieved at the following deposition parameters: 1200 W, N/Ar = 1.8/0.06 L/h = 30, 0.8 Pa, 320 s, and 100°C. At temperatures 700–800°C, the mutual diffusion of titanium and silicon atoms through the interface leads to the active nucleation, the formation of nanocrystals and low-resistance metallization layers. X-ray diffraction shows that, during annealing at 700°C (30 min, Ar), the formation of phase TiSi_2 due to the diffusion of Ti atoms into silicon is twice more intense than the formation of Ti_5Si_3 due to the diffusion of silicon atoms into titanium as a result of high hardness of titanium. The average sizes of TiSi_2 decreases from 7.1 to 5.6 nm at 750°C due to the crystallization of the nuclei and increase to 9.2 nm at 800°C.


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