Density Matrix Analysis and Simulation of Electronic Excitations in Conjugated and Aggregated Molecules

2002 ◽  
Vol 102 (9) ◽  
pp. 3171-3212 ◽  
Author(s):  
Sergei Tretiak ◽  
Shaul Mukamel
1988 ◽  
Vol 125 (2-3) ◽  
pp. 211-223 ◽  
Author(s):  
K. Wynne ◽  
M. Müller ◽  
D. Brandt ◽  
J.D.W. Van Voorst

Molecules ◽  
2021 ◽  
Vol 26 (14) ◽  
pp. 4245
Author(s):  
Evgenii Titov

Azobenzene-containing molecules may associate with each other in systems such as self-assembled monolayers or micelles. The interaction between azobenzene units leads to a formation of exciton states in these molecular assemblies. Apart from local excitations of monomers, the electronic transitions to the exciton states may involve charge transfer excitations. Here, we perform quantum chemical calculations and apply transition density matrix analysis to quantify local and charge transfer contributions to the lowest electronic transitions in azobenzene dimers of various arrangements. We find that the transitions to the lowest exciton states of the considered dimers are dominated by local excitations, but charge transfer contributions become sizable for some of the lowest ππ* electronic transitions in stacked and slip-stacked dimers at short intermolecular distances. In addition, we assess different ways to partition the transition density matrix between fragments. In particular, we find that the inclusion of the atomic orbital overlap has a pronounced effect on quantifying charge transfer contributions if a large basis set is used.


2006 ◽  
Vol 110 (5) ◽  
pp. 1775-1782 ◽  
Author(s):  
Vladimir Lukeš ◽  
Tibor Pálszegi ◽  
Franz Milota ◽  
Jaroslaw Sperling ◽  
Harald Friedrich Kauffmann

2008 ◽  
Vol 07 (04) ◽  
pp. 869-877 ◽  
Author(s):  
YI ZHAO

Feynman and Vernon path integral approach is adopted to investigate electron transfer dynamics in donor–bridge–acceptor molecules under dissipative environments. Especially, we focus on the solvent effect on the superexchange process of electron transfer. The results reveal that at high enough bridge energies or low enough temperature, electron can transfer with a superexchange mechanism no matter whether solvent is incorporated or not. However, the superexchange changes from coherent to incoherent limits when the dissipative strength increases, and electron transfer rates are much dependent on the dissipative strength.


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