scholarly journals Scattering of multicomponent polymer blends

Author(s):  
Henrich Frielinghaus

AbstractThe random phase approximation for polymer blends was developed by H. Benoît and described small angle scattering functions as well as mean field phase boundaries. It is a pure mean field theory that loses validity close to the real phase boundaries due to strong fluctuations. However, it gives a very clear roadmap about phase diagrams and scattering functions. A simplification of the random phase approximation is discussed that comes into effect when several polymers are mixed that involve a rather low number of chemically different repeat units. Then, the correlation functions of the same repeat unit pairs can be added up in a specific way such that the overall complexity for the calculations is reduced. The scattering functions and mean field phase boundaries are discussed within this concept. Graphical abstract

2001 ◽  
Vol 694 (1-2) ◽  
pp. 249-268 ◽  
Author(s):  
P. Ring ◽  
Zhong-yu Ma ◽  
Nguyen Van Giai ◽  
D. Vretenar ◽  
A. Wandelt ◽  
...  

1989 ◽  
Vol 40 (1) ◽  
pp. 399-406 ◽  
Author(s):  
J. A. McNeil ◽  
R. J. Furnstahl ◽  
E. Rost ◽  
J. R. Shepard

Polymer ◽  
1986 ◽  
Vol 27 (12) ◽  
pp. 1935-1942 ◽  
Author(s):  
A.Ziya Akcasu ◽  
M. Benmouna ◽  
H. Benoit

1996 ◽  
Vol 05 (03) ◽  
pp. 511-520
Author(s):  
ABHIJIT BHATTACHARYYA

The temperature dependence of σ and ω meson effective masses due to the presence of Δ-baryon has been studied. Starting from the Walecka model, containing both nucleon and Δ, the temperature dependence of effective masses of nucleon and Δ have been calculated at the Mean Field (MF) level. These results have been used to calculate the contribution to the effective masses of σ and ω from both [Formula: see text]- and [Formula: see text]-loops in Random Phase Approximation (RPA). The results are quite interesting. The σ-meson mass increases due to the [Formula: see text] loop whereas it decreases due to [Formula: see text]-loop with temperature. Further, the change in σ-meson mass due to [Formula: see text]-loop is much more compared to that due to [Formula: see text]-loop. For the ω-meson, both the loops are responsible for the increase in mass with temperature.


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