Computational Studies on the Erosion Process in a Magnetron Sputtering System with a Ferromagnetic Target

1998 ◽  
Vol 37 (Part 1, No. 3A) ◽  
pp. 965-969 ◽  
Author(s):  
Shunji Ido ◽  
Takeshi Suzuki ◽  
Mieko Kashiwagi
Keyword(s):  
Magnetron Sputtering ◽  
Computational Studies ◽  
Erosion Process ◽  
Sputtering System

Computational Studies of Plasma Generation and Control in a Magnetron Sputtering System

1999 ◽  
Vol 38 (Part 1, No. 7B) ◽  
pp. 4450-4454 ◽  
Author(s):  
Shunji Ido ◽  
Mieko Kashiwagi ◽  
Mikihiko Takahashi
Keyword(s):  
Magnetron Sputtering ◽  
Computational Studies ◽  
Plasma Generation ◽  
And Control ◽  
Sputtering System

scholarly journals Controlling Film Thickness Distribution by Magnetron Sputtering with Rotation and Revolution

Coatings ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 599
Author(s):  
Handan Huang ◽  
Li Jiang ◽  
Yiyun Yao ◽  
Zhong Zhang ◽  
Zhanshan Wang ◽  
...  
Keyword(s):  
Magnetron Sputtering ◽  
Film Thickness ◽  
Multilayer Film ◽  
Thickness Distribution ◽  
Parabolic Cylinder ◽  
Particle Model ◽  
Planetary Motion ◽  
X Rays ◽  
X Ray ◽  
Sputtering System

The laterally graded multilayer collimator is a vital part of a high-precision diffractometer. It is applied as condensing reflectors to convert divergent X-rays from laboratory X-ray sources into a parallel beam. The thickness of the multilayer film varies with the angle of incidence to guarantee every position on the mirror satisfies the Bragg reflection. In principle, the accuracy of the parameters of the sputtering conditions is essential for achieving a reliable result. In this paper, we proposed a precise method for the fabrication of the laterally graded multilayer based on a planetary motion magnetron sputtering system for film thickness control. This method uses the fast and slow particle model to obtain the particle transport process, and then combines it with the planetary motion magnetron sputtering system to establish the film thickness distribution model. Moreover, the parameters of the sputtering conditions in the model are derived from experimental inversion to improve accuracy. The revolution and rotation of the substrate holder during the final deposition process are achieved by the speed curve calculated according to the model. Measurement results from the X-ray reflection test (XRR) show that the thickness error of the laterally graded multilayer film, coated on a parabolic cylinder Si substrate, is less than 1%, demonstrating the effectiveness of the optimized method for obtaining accurate film thickness distribution.

The synthesis of CrSiN film deposited using magnetron sputtering system

2005 ◽  
Vol 200 (1-4) ◽  
pp. 1026-1030 ◽  
Author(s):  
H.Y. Lee ◽  
W.S. Jung ◽  
J.G. Han ◽  
S.M. Seo ◽  
J.H. Kim ◽  
...  
Keyword(s):  
Magnetron Sputtering ◽  
Sputtering System

Effects of dopant (Al, Ga, and In) on the characteristics of ZnO thin films prepared by RF magnetron sputtering system

2010 ◽  
Vol 10 (3) ◽  
pp. S463-S467 ◽  
Author(s):  
Kyu Ung Sim ◽  
Seung Wook Shin ◽  
A.V. Moholkar ◽  
Jae Ho Yun ◽  
Jong Ha Moon ◽  
...  
Keyword(s):  
Thin Films ◽  
Magnetron Sputtering ◽  
Rf Magnetron Sputtering ◽  
Zno Thin Films ◽  
Sputtering System

Structural Evolution Upon Annealing of Multi-Layer Si/Fe Thin Films Prepared by Magnetron Sputtering

2007 ◽  
Vol 561-565 ◽  
pp. 1161-1164
Author(s):  
Xiao Na Li ◽  
Bing Hu ◽  
Chuang Dong ◽  
Xin Jiang
Keyword(s):  
Thin Films ◽  
Magnetron Sputtering ◽  
Room Temperature ◽  
Structural Evolution ◽  
Radio Frequency Magnetron Sputtering ◽  
Transmission Electron ◽  
Direct Band ◽  
The Stability ◽  
Sputtering System

Fe/Si multi-layer films were fabricated on Si (100) substrates utilizing radio frequency magnetron sputtering system. Si/β-FeSi2 structure was found in the films after the deposition. Structural characterization of Fe-silicide sample was performed by transmission electron microscopy, to explore the dependence of the microstructure of β-FeSi2 film on the preparation parameters. It was found that β-FeSi2 particles were formed after the deposition without annealing, whose size is less than 20nm ,with a direct band-gap of 0.94eV in room temperature. After annealing at 850°C, particles grow lager, however the stability of thin films was still good.

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