Statistical theory for self-condensing vinyl polymerization system with any initial distribution

2013 ◽  
Vol 43 (11) ◽  
pp. 1505-1511 ◽  
Author(s):  
XiaoZhong HONG ◽  
Fang GU ◽  
HaiJun WANG ◽  
XinWu BA
2015 ◽  
Vol 58 (12) ◽  
pp. 1875-1883 ◽  
Author(s):  
Xiaozhong Hong ◽  
Zuofei Zhao ◽  
Haijun Wang ◽  
Xinwu Ba

Polymer ◽  
2012 ◽  
Vol 53 (22) ◽  
pp. 5010-5015 ◽  
Author(s):  
Lingjuan Li ◽  
Xin Shu ◽  
Jin Zhu

Polymer ◽  
2010 ◽  
Vol 51 (13) ◽  
pp. 2857-2863 ◽  
Author(s):  
Xiao-hui Liu ◽  
You-mei Bao ◽  
Xiu-lan Tang ◽  
Yue-sheng Li

2009 ◽  
Vol 131 (7) ◽  
pp. 074101 ◽  
Author(s):  
Zuo-Fei Zhao ◽  
Hai-Jun Wang ◽  
Xin-Wu Ba

2015 ◽  
Vol 58 (9) ◽  
pp. 1478-1488
Author(s):  
Zuofei Zhao ◽  
Yuanfeng Li ◽  
Ning Yao ◽  
Haijun Wang

Author(s):  
Harry A. Atwater ◽  
C.M. Yang ◽  
K.V. Shcheglov

Studies of the initial stages of nucleation of silicon and germanium have yielded insights that point the way to achievement of engineering control over crystal size evolution at the nanometer scale. In addition to their importance in understanding fundamental issues in nucleation, these studies are relevant to efforts to (i) control the size distributions of silicon and germanium “quantum dots𠇍, which will in turn enable control of the optical properties of these materials, (ii) and control the kinetics of crystallization of amorphous silicon and germanium films on amorphous insulating substrates so as to, e.g., produce crystalline grains of essentially arbitrary size.Ge quantum dot nanocrystals with average sizes between 2 nm and 9 nm were formed by room temperature ion implantation into SiO2, followed by precipitation during thermal anneals at temperatures between 30°C and 1200°C[1]. Surprisingly, it was found that Ge nanocrystal nucleation occurs at room temperature as shown in Fig. 1, and that subsequent microstructural evolution occurred via coarsening of the initial distribution.


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