Theory of non-Condon emission from the interchain exciton in conjugated polymer aggregates
J. Chem. Phys. 126, 191102 (2007); doi:10.1063/1.2741250
Published 17 May 2007
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The authors present here a simple analysis that explains the apparent strengthening of electron phonon interaction upon aggregation in conjugated polymer materials. The overall scheme is that of an intermolecular Herzberg-Teller effect whereby sidebands of a forbidden transition are activated by oppositely phased vibrations. The authors show that upon aggregation, the 0-0 emission becomes symmetry forbidden and the apparent redshift and remaining vibronic structure are due to sideband (0-1,0-2, etc.) emission. At higher temperatures, the 0-0 peak is due to thermal population in a higher lying even-parity vibronic state rather than direct emission from the odd-paritied lowest intermolecular vibronic state.
©2007 American Institute of Physics
| History: | Received 21 November 2006; accepted 25 April 2007; published 17 May 2007 |
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http://link.aip.org/link/?JCPSA6/126/191102/1 |
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0021-9606 (print)
1089-7690 (online)
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- For this, we use the following parameters: S=1,
![[h-bar]](http://scitation.aip.org/stockgif3/planck.gif)
=0.18 eV, Vab=![[h-bar]](http://scitation.aip.org/stockgif3/planck.gif)
/3, and
a=
b=0 as discussed in the text.








