Application of a photodimerizable probe to the forced Rayleigh scattering technique for measurement of self-diffusion of polymer chains

Polymer ◽  
1986 ◽  
Vol 27 (11) ◽  
pp. 1705-1708 ◽  
Author(s):  
Qui Tran-Cong ◽  
Taihyun Chang ◽  
Charles C. Han ◽  
Yasunori Nishijima
1987 ◽  
Vol 115 (2) ◽  
pp. 545-550 ◽  
Author(s):  
William D Dozier ◽  
Mahn Won Kim ◽  
Paul M Chaikin

1984 ◽  
Vol 17 (1) ◽  
pp. 115-117 ◽  
Author(s):  
Taihyun Chang ◽  
Hyuk Yu

RSC Advances ◽  
2014 ◽  
Vol 4 (64) ◽  
pp. 34204-34209 ◽  
Author(s):  
Ernv Wang ◽  
Jidong Yang ◽  
Donghai Yu

EV-EMO system. CEMO(1–8) 0, 0.4, 1.0, 1.5, 2.3, 3.2, 3.8, 4.2 μg mL−1; CEV: 1.2 × 10−5 mol L−1; pH 7.0.


1984 ◽  
Vol 17 (4) ◽  
pp. 782-792 ◽  
Author(s):  
Jeffrey A. Wesson ◽  
Icksam Noh ◽  
Toshiaki Kitano ◽  
Hyuk Yu

2012 ◽  
Vol 16 (12) ◽  
pp. 1276-1284 ◽  
Author(s):  
Xiao Ying ◽  
Xiao-Yan Long ◽  
Mian HR Mahmood ◽  
Quan-Yuan Hu ◽  
Hai-Yang Liu ◽  
...  

The first hyperpolarizabilities, βHRS, of corrole derivatives have been measured by using Hyper–Rayleigh Scattering technique. The results showed that βHRS of corroles could be greatly enhanced by modifying its periphery with donor–acceptor groups. Maximum value reaches 354 × 10-30 esu at an incident wavelength of 1500 nm. βHRS of investigated corroles were also calculated with the Zerner's intermediate neglect of differential overlap/configuration interaction/sum-over-states method. The calculated and experimental results are in good agreement and conclude that βHRS arises mainly from the charge transfer along molecule's non-symmetrical axis and strong coupling between two different excited states of the Soret band.


2005 ◽  
Vol 73 (1) ◽  
pp. 5-15 ◽  
Author(s):  
Jean K. Platten

In the first part of the paper, we recall what the Soret effect is, together with its applications in science and industry. We emphasize the need to have a reliable data base for the Soret coefficient. Next we review the different techniques to measure the Soret coefficient (elementary Soret cell, beam deflection technique, thermal diffusion forced Rayleigh scattering technique, convective coupling and, in particular, the onset of convection in horizontal layers and the thermogravitational method). Results are provided for several systems, with both negative and positive Soret coefficients, and comparison between several laboratories are made for the same systems. We end with “benchmark” values of the Soret coefficient for some organic liquid mixtures of interest in the oil industry and to which all future new techniques should refer before gaining confidence. We conclude that correct values of the Soret coefficient can be obtained in earth conditions and we deny the need to go to microgravity.


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