The Homogeneous Design of Large Area Film Hollow Cathode Plasma Graft Polymerization

2013 ◽  
Vol 567 ◽  
pp. 45-51
Author(s):  
Yi Fang Wen ◽  
Chuang Chen ◽  
Xin Chen ◽  
Yan Nian Rui ◽  
Ning Ding

CRFHCP RF hollow cathode plasma graft polymerization has characteristics of discharge density, high discharging efficiency, good surface modification effect, discharge area and regional separation, applies to modify large area thin film material surface. The uniformity modifying large area plasma material surface is the technical difficulty related technical personnel has been concerned with, the key point restricting HCRFCP technology industrialization application too. This paper analyzes influence factors of the large area thin film materials plasma graft polymerization uniformity; applies simulation software and mathematical models; makes optimized design to the hollow cathode discharge electrodes and graft polymerization distributing pipe. The experiment proved, the uniformity processing large area battery diaphragm is better to apply the hollow cathode plasma graft polymerization, and is suitable for industrial application.

2016 ◽  
Vol 693 ◽  
pp. 1054-1060
Author(s):  
Yi Fang Wen ◽  
Yan Nian Rui ◽  
Hong Wei Wang

The graft polymerization in radio frequency hollow cathode plasma (RFHCP) is suitable for the surface modification of large-area thin film materials. The homogeneity of plasma surface modification of large-area thin film materials has always been paid close attention, and it is also the key factor affecting the industrialized applications of the technique. However, the homogeneity of plasma surface modification is thought to depend greatly on the distribution of discharge gas. In this paper, a finite element model is proposed to discuss the flow of discharge gas in hollow cathode plasma. The concentration distribution of the discharge gas has been discussed by the combination of numerical simulation of fluid distribution and pipe flow theory based on the investigation of the transport property of gas under vacuum. Comparisons between available experiments have also been performed to validate the applicability and practicability of the proposed model.


2013 ◽  
Vol 819 ◽  
pp. 344-349
Author(s):  
Yi Fang Wen ◽  
Yan Nian Rui ◽  
Chuang Chen ◽  
Hong Wei Wang

The discharge of RF hollow cathode far zone plasma has advantages of high ion concentration, easy to implement the processing of a large area, given more and more attention. The characteristics of hollow cathode plasma flow have a great relationship with the hollow cathode nozzle structure. How to design the hollow cathode nozzle discharge structure accurately and conveniently is the key problem of the hollow cathode far plasma surface treatment. This article builds a hollow cathode plasma discharge self-consistent model; derive the relationship between the discharge current of the hollow cathode plasma and the hollow cathode nozzle structure. Optimize the design of the hollow cathode discharge structure using discharge particle simulation software, to achieve a fast and accurate design and the purpose of efficient plasma surface modification.


2005 ◽  
Vol 486-487 ◽  
pp. 157-160
Author(s):  
Min Kyu Yang ◽  
Hyu Seung Yang ◽  
Jong Ku Park ◽  
Keun Ryu ◽  
Yong Bok Lee ◽  
...  

The self-lubricating composite films were deposited on Inconel 718 by Hollow Cathode Plasma Jet (HCPJ). These composite materials consist of chrome nickel alloy matrix and Ag, BaF2/CaF2 solid lubricants. The Cr2O3-NiCr-Ag composite thin film was crystallized and had the main peaks of Cr2O3 (012) and Ag (111). The deposition rate of 200 nm /min by HCPJ was much faster than the ordinary R.F planar magnetron sputtering. The surface roughness of coated shaft was 30 nm.


The review deals with the electronic properties and recent applications of amorphous silicon (a-Si), which can be regarded as the first member of a new generation of electronically viable thin-film materials. After a brief introduction to the structure and the distribution of electronic states in a-Si the preparation of the material by the decomposition of silane in a radio-frequency glow discharge is discussed. The presence of hydrogen in the deposition process is of crucial importance; saturation of defect states, particularly of dangling bonds in the growing structure, leads to a material with a remarkably low density of gap states. Effective substitutional doping from the gas phase now becomes possible with wide-ranging control of the electronic properties. A brief discussion of the doping mechanism in amorphous solids is followed by a summary of carrier transport mechanisms in a-Si, investigated by fast transient techniques. The possibility of doping in a-Si has removed a major limitation in the a-semiconductor field and has, during the past 10 years, led to an upsurge in applied interest in this electronically controllable thin film material. A summary of the present state of applied developments, many already in industrial production, is given. Two groups are discussed in some detail. The first, the photovoltaic development, is based on the a-Si p–i–n junction, and forms part of a wide range of consumer products, but larger area photovoltaic panels are now in production. In the second major development a-Si field effect transistors are used as the addressable elements in large area liquid crystal displays. Remarkable progress has been made with thin film colour displays for small portable television sets. The use of a-Si elements in addressable linear image sensing arrays for telefax applications, coupled with a-Si high-voltage transistor arrays in the associated printers, represents an important step towards an integrated a-Si technology in large-area applications.


1991 ◽  
Vol 9 (4) ◽  
pp. 2374-2377 ◽  
Author(s):  
H. Koch ◽  
L. J. Friedrich ◽  
V. Hinkel ◽  
F. Ludwig ◽  
B. Politt ◽  
...  

2010 ◽  
Vol 205 (5) ◽  
pp. 1532-1535 ◽  
Author(s):  
Jeonghee Cho ◽  
Jack Yang ◽  
Haejung Park ◽  
Se-Geun Park

1996 ◽  
Vol 262 (1-2) ◽  
pp. 89-97 ◽  
Author(s):  
Th. Schurig ◽  
S. Menkel ◽  
Z. Quan ◽  
J. Beyer ◽  
B. Güttler ◽  
...  

The Thin Film Transistor (TFT) is the key active components of emerging large area and flexible microelectronics (LAFM) which includes a flexible display, robotics skin, sensor & disposable electronics. Different semiconducting or organic conducting materials could be used in the fabrication of TFTs. The material used for the active layer also influences the performance of the TFT uniquely[1]. Silicon based thin film transistors have made possible the development of the active-matrix liquid crystal display within cell-touch technology [2,3,4]. Modern-day simulation software does not support the older SPICE code models, and rather rely on the new drag and drop concepts. The TFT(Thin Film Transistor) Model device wasn't readily available on the LT-Spice Tool which was simulated and the circuit level simulation for basic gates using the TFT was carried out successfully. The model symbol shall be useful for analysis and simulation of the TFT based circuits which require continuous behavioral study and analysis. For a device to be simulated that way, a “.lib” file containing a symbol of the device is necessary. This paper focuses on circuit-level simulation of user-defined device parameters from reported experimental data.


Sign in / Sign up

Export Citation Format

Share Document