The theoretical calculations, however, could not account for the apparent offset
seen in Fig. 21b. It has been speculated that this off-set might be traced back to a
coherent coupling mechanism contributing to the optical line width [9]. Finally,
theoretical results for 1 in PMMA have yielded an excellent agreement between the
Fo ¨rster screening factor 1/n
4 and a screening factor obtained by considering a cavity
enclosing the dyad inside the PMMA dielectric environment [132].
Acknowledgement The contributions of our co-workers Burkhard Fu ¨ckel, Long Chen, Gregor
Diezemann, Gerald Hinze, Ting Ren, Daniel Wenzlik, Mara Werwie and Xiangxing Xu are
gratefully acknowledged.
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Fig. 24 Coupling of a p-terphenyl to the PDI chromophore (left). Shown are the isosurfaces of
(a) the transition density and (b) the difference density. The calculations were performed with the
CC2 method and a SVP basis set. Reproduced with permission from [3]. Copyright 2008 American
Institute of Physics
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