Excitons at Polymer Interfaces

2013 ◽  
pp. 295-331
Author(s):  
Neil Greenham
Keyword(s):  
1988 ◽  
Vol 49 (C5) ◽  
pp. C5-49-C5-59 ◽  
Author(s):  
P. S. HO ◽  
R. HAIGHT ◽  
R. C. WHITE ◽  
B. D. SILVERMAN

2006 ◽  
Vol 110 (22) ◽  
pp. 10602-10605 ◽  
Author(s):  
Shane E. Harton ◽  
Frederick A. Stevie ◽  
Zhengmao Zhu ◽  
Harald Ade

Langmuir ◽  
2005 ◽  
Vol 21 (14) ◽  
pp. 6157-6160 ◽  
Author(s):  
Tadanori Koga ◽  
J. L. Jerome ◽  
Y.-S. Seo ◽  
M. H. Rafailovich ◽  
J. C. Sokolov ◽  
...  

2006 ◽  
Vol 39 (26) ◽  
pp. 9396-9401 ◽  
Author(s):  
Mark A. Even ◽  
Chunyan Chen ◽  
Jie Wang ◽  
Zhan Chen

2002 ◽  
Vol 56 (4) ◽  
pp. 509-514 ◽  
Author(s):  
Xiaohua Yi ◽  
Karen Nerbonne ◽  
John Pellegrino

We present an experimental method for measuring diffusion of lubricants (or any highly viscous fluid) in polymers using Fourier transform infrared (FT-IR) attenuated total reflection (ATR) spectroscopy. Unlike the conventional FT-IR ATR diffusion measurement, in which a polymer sample is sandwiched between the penetrant and an internal reflection element (IRE), in this method, a thin layer of penetrant (for example, a lubricant) is sandwiched between the IRE and the polymer sample. This allows accurate control and measurement of the thickness of the lubricant layer, which, in turn, facilitates subsequent data analysis. The diffusion is studied by monitoring the time-resolved change in absorbance of either a unique polymer or penetrant band. A feature of this new method is that it can provide an estimate of solubility, as well as an estimate of the diffusivity of the penetrant in the polymer. Using this method, we studied the diffusion of mineral oil and a commercial fluorocarbon ether lubricant (Krytox® 143AC‡) in poly(propylene) (PP) film at room temperature. The experimental data was modeled using a Fickian model with impermeable and saturated boundary conditions applied at the IRE/lubricant and lubricant/polymer interfaces, respectively. The diffusivity and solubility of mineral oil in PP were found to be 1.34 ± 0.35 (×10−10) cm2/s and 0.77 ± 0.13 (×10−2) g/g of PP, respectively. The current model was unable to quantitatively describe the diffusion of the Krytox® 143AC in the PP, possibly due to excessive swelling.


1990 ◽  
Vol 22 (4) ◽  
pp. 265-301 ◽  
Author(s):  
A. Lechtenboehmer ◽  
H. G. Moneypenny ◽  
F. Mersch
Keyword(s):  

2005 ◽  
Vol 30 (8-9) ◽  
pp. 939-947 ◽  
Author(s):  
Christopher W. Macosko ◽  
Hyun K. Jeon ◽  
Thomas R. Hoye
Keyword(s):  

2014 ◽  
Vol 187 (2) ◽  
pp. 227-238
Author(s):  
Siow Ling Ho ◽  
Shailendra P. Joshi ◽  
Andrew A. O. Tay

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