scholarly journals Charge symmetry broken complex coacervation

2020 ◽  
Vol 2 (4) ◽  
Author(s):  
Arghya Majee ◽  
Markus Bier ◽  
Ralf Blossey ◽  
Rudolf Podgornik
ACS Omega ◽  
2020 ◽  
Vol 5 (51) ◽  
pp. 33064-33074
Author(s):  
Preeti Tiwari ◽  
Indu Bharti ◽  
Himadri B Bohidar ◽  
Shabina Quadir ◽  
Mohan C Joshi ◽  
...  

2021 ◽  
Vol 126 (23) ◽  
Author(s):  
Debra J. Audus ◽  
Samim Ali ◽  
Artem M. Rumyantsev ◽  
Yuanchi Ma ◽  
Juan J. de Pablo ◽  
...  

2012 ◽  
Vol 627 ◽  
pp. 770-774
Author(s):  
Xiao Mei Wang ◽  
Bao Bao Zhao ◽  
Cheng Rong Zhang

Microcapsules were prepared using the complex coacervation method with nano anatase TiO2 as the core material, gelatin/Arabia gum as the wall material, while dispersing TiO2 into the reaction solution using the ultrasonic. The prepared microcapsules can be finished into textiles such as the polypropylene nonwovens, and the microcapsules in the textiles gradually fracture and the anatase TiO2 was released, which would facilitate photo-degradation of the polypropylene nonwovens when exposed in sunlight. The microcapsules size was used as the process optimization evaluation index, and the quadratic general revolving combination design was used to conduct the experiments for obtaining the optimum ultrasonic conditions, and the other progress parameters were the same that used in our early microcapsule preparation. The obtained optimal process for ultrasound is: ultrasonic time is 17min; ultrasonic power is 74W and ultrasound temperature 60 °C.


2013 ◽  
Vol 141 (1) ◽  
pp. 215-222 ◽  
Author(s):  
Seyed Mohammad Hashem Hosseini ◽  
Zahra Emam-Djomeh ◽  
Seyed Hadi Razavi ◽  
Ali Akbar Moosavi-Movahedi ◽  
Ali Akbar Saboury ◽  
...  

1982 ◽  
Vol 115 (3) ◽  
pp. 171-173 ◽  
Author(s):  
L.N. Bogdanova ◽  
V.E. Markushin ◽  
V.S. Melezhik ◽  
L.I. Ponomarev

2011 ◽  
Vol 36 (2) ◽  
pp. 185-190 ◽  
Author(s):  
D.F. SILVA ◽  
C.S. FAVARO-TRINDADE ◽  
G.A. ROCHA ◽  
M. THOMAZINI
Keyword(s):  

1992 ◽  
Vol 07 (32) ◽  
pp. 3037-3043 ◽  
Author(s):  
T. GOLDMAN ◽  
J.A. HENDERSON ◽  
A.W. THOMAS

In generating a charge-symmetry breaking potential using ρ-ω mixing it is usually assumed that the mixing amplitude is constant (at the on-mass-shell value). Since the exchanged meson is actually far off-shell one must question the validity of this assumption. By constructing a simple quark model in which the mixing is generated by the u-d quark mass difference, we find that the assumption seems to be a very poor one.


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