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1.
J Phys Chem A ; 121(8): 1597-1606, 2017 Mar 02.
Artigo em Inglês | MEDLINE | ID: mdl-28140598

RESUMO

The lowest two electronically excited singlet states of indole and its derivatives are labeled as La or Lb, based on the orientation of the transition dipole moment (TDM) and the magnitude of the permanent electric dipole moment. Rotationally resolved electronic Stark spectroscopy in combination with high level ab initio calculations offers the possibility to determine these characteristics and thus the electronic nature of the excited states. In the present contribution this approach was pursued for the systems 4- and 6-fluoroindole and the results compared to the previously investigated system 5-fluoroindole. Changing the position of the fluorine atom from 5 to 4 or 6 is accompanied by an increasing amount of La character in the S1 state. This dramatically influences the orientation of the TDM and erases its ability to be a reasonable identifier of the nature of the excited states for both molecules. However, for 4-fluoroindole, where the influence of the La is weak, the nature of the S1 state can still be assigned to be mainly Lb based on the excited state dipole moment. For 6-fluoroindole, this is not the case anymore, and the La/Lb nomenclature completely breaks down due to heavily mixed excited states.

2.
J Phys Chem B ; 120(34): 8845-62, 2016 09 01.
Artigo em Inglês | MEDLINE | ID: mdl-27490865

RESUMO

Förster resonance energy transfer (FRET) is analyzed in terms of distance- and orientation-dependent interactions between the transition dipole moments of the involved donor and acceptor molecules. However, the ideal dipole approximation (IDA) is known to fail at short donor-acceptor distances. In this work, we model FRET in a Cy5- and Alexa Fluor 488-labeled double-stranded RNA by means of combined molecular dynamics (MD) simulations and quantum-chemical calculations involving the IDA as well as the more sophisticated monomer transition density (MTD) approach. To this end, the relaxed ground-state geometries of the dyes were fitted to the MD-based structures. Although substantial deviations between IDA and MTD results can be observed for individual snapshots, the statistical impact of the failure on the FRET rates is negligible in the chosen examples. Our results clearly demonstrate that the IDA-based Förster model can still be applied to systems with small donor-acceptor distances, provided that the dyes are not trapped in arrangements with a high IDA failure and that the distribution of the relative transition dipole orientations is fairly isotropic.


Assuntos
Carbocianinas/química , Transferência Ressonante de Energia de Fluorescência , Corantes Fluorescentes/química , Simulação de Dinâmica Molecular , RNA de Cadeia Dupla/química , Estrutura Molecular , Teoria Quântica
3.
J Chem Theory Comput ; 11(9): 4316-27, 2015 Sep 08.
Artigo em Inglês | MEDLINE | ID: mdl-26575926

RESUMO

BODIPY-based excitation energy transfer (EET) cassettes are experimentally extensively studied and serve as excellent model systems for the investigation of photophysical processes, since they occur in any photosynthetic system and in organic photovoltaics. In the present work, the EET rates in five BODIPY-based EET cassettes in which anthracene serves as the donor have been determined, employing the monomer transition density approach (MTD) and the ideal dipole approximation (IDA). To this end, a new computer program has been devised that calculates the direct and exchange contributions to the excitonic coupling (EC) matrix element from transition density matrices generated by a combined density functional and multireference configuration interaction (DFT/MRCI) calculation for the monomers. EET rates have been calculated according to Fermi's Golden Rule from the EC and the spectral overlap, which was obtained from the calculated vibrationally resolved emission and absorption spectra of donor and acceptor, respectively. We find that the direct contribution to the EC matrix element is dominant in the studied EET cassettes. Furthermore, we show that the contribution of the molecular linker to the EET rate cannot be neglected. In our best fragment model, the molecular linker is attached to the donor moiety. For cassettes in which the transition dipole moments of donor and acceptor are oriented in parallel manner, our results confirm the experimental findings reported by Kim et al. [J. Phys. Chem. A 2006, 110, 20-27]. In cassettes with a perpendicular orientation of the donor and acceptor transition dipole moments, dynamic effects turn out to be important.

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